What is Shear Stress? | Its All Important Concepts

ezgif 4 85c0bc9cff
  • When force transmits from one body to another, forces parallel to the surface are experienced by the body, such kind of forces produce shear stress.
  • It is vital to know about the shear stresses acting on the material while designing the product. Shear failure is the most common failure which occurs due to inappropriate consideration of shear forces.

Shear Stress Definition

  • When the applied force is parallel/tangential to the surface area of application, then the stress produced is known as shear stress.
  • Here application of force is tangential to the surface of application.
  •  A component of the stress tensor in the direction parallel to the area of application.
  • Shear stress also occurs in axial loading, bending, etc.

Shear Stress Formula

 Shear Stress= Force imposed parallel to the area/ Area of cross-section

ezgif 4 85c0bc9cff

What is Shear Stress Units ?

Unit of shear stress is N/m2 or Pa.

In industries, the unit used to measure shear stress is N/mm2 or MPa (Mega Pascal)

Shear Stress Symbol | Shear Stress tau

The symbol used to represent shear stress is τ (Tau). It is also represented by T.

Shear Stress Diagram

Shear Stress Diagram
Shear Stress Diagram

Shear Stress Notation

  • Symbol τ is used to represent shear stress.
  • To show the applied force and direction of the application area, subscripts are used with the symbol τ as τij.
  • Where i represent the direction of the surface plane on which it is being applied (perpendicular to the surface), and j represents the applied force’s direction.
  • Thus, τij= Shear stress acting on the i-surface in j-direction.

          τji= Shear stress acting on the j-surface in i-direction.

  • We can write it as:
ezgif 4 237490c9d9

Shear Stress Direction

In 2 Dimensions:

2 1
Shear Stress Direction
  • In the vector form, shear stress is the ratio of a parallel component of force applied to the unit normal vector of area.

                  τ= F / A

In 3 Dimensions:

  • In naming xy, which is in the subscript form (subscript convention), index x represents the direction of a vector perpendicular to the application area, and y represents the direction of applied force.
  • In the following figure, it is represented for all three axes.
Shear Stress Directions
Shear Stress Direction

Any of the shear stress can be represented as follow:           

ezgif 4 ba9ebff8fa

Shear Stress Sign Convention

When the shear stress is applied on a surface along the principal axis, the adjacent perpendicular axis experiences the equal amount of shear stress in the opposite direction known as complementary shear stress as shown in the figure:

Complementary Shear Stress
Complimentary Shear Stress
  • Shear stress is positive if the shear force applied along the x-axis is in the right direction or clockwise.

Similarly, Shear stress is positive if the shear force applied along the y-axis is in an upward direction or it is counterclockwise.

  • Shear stress is negative if the shear force applied along the x-axis is in the left direction or in counterclockwise.

Similarly, Shear stress is negative if the shear force applied along the y-axis is in a downward direction or it is clockwise.

  • Half arrowheads are used to represent shear stress.
Shear Stress Sign Convention
Shear Stress Sign Convention

Shear Strain

  • When the shear stress is applied on a surface, deformation is produced in the material. So, the ratio of deformation to the original length perpendicular to the member’s axes is known as shear strain. It is denoted by γ.
  • It is also defined as the tangent of the strain angle ө.
  • Shear Strain= del l/ h = tangent(Ө)
Shear Strain
Shear Strain
ezgif 4 ba9ebff8fa 1

Shear Stress and Shear Strain

  • It is noted that shear strain is dependent on shear stress. The relation is expressed as
ezgif 4 93f4cad4cc

Modulus of Rigidity | Shear Stress Modulus | Shear Modulus of Rigidity

  • The proportionality constant G is known as Modulus of Rigidity or Shear Stress Modulus or Shear Modulus of Rigidity.
  • Thus,

     Modulus of Rigidity = Shear Stress/ Shear Strain

ezgif 4 b4bd1d61f4
  • In most of the metals, G is about 0.4 times of Young’s Modulus of Elasticity.

For isotropic materials, Modulus of Rigidity and Modulus of Elasticity is related to each other according to

      Y = 2*G* (1+ ʋ)

Where, Y= Modulus of Elasticity

             G= Modulus of Rigidity

             ʋ= Poisson’s Ratio

Shear Strength

  • Shear strength is the maximum value of shear stress that can resist failure due to shear stress.
  • It is a significant parameter while designing and manufacturing machines.
  • Example: While designing bolts and rivets, it is indispensable to know about the material’s shear strength.

Shear Stress vs Normal Stress

 Shear StressNormal Stress
1.Force applied is parallel to the surface on which it is being appliedForce applied is perpendicular to the surface on which it is being applied.
2.Force vector and area vector are perpendicular to each otherForce vector and area vector are parallel to each other.

 Shear Stress from Torque | Shear Stress Due to Torsion

  • Torque is a rotational form of force which makes the object to rotate around an axis. When this torque is applied on a deformable body, it generates shear stress in that body, making that body twist around an axis, known as torsion.
  • This type of stress is significant in shafts. The stresses or deformations induced in the shaft due to this torsion are shear kinds of stresses.
  • The shear strain produced in the following shaft of radius r is represented as follows:

γ= rdө/dz

Shear Stress due to Torque
Shear Stress due to Torque

Thus, the shear stress produced is represented by

ezgif 4 8bc39f719b

Shear Stress Fluid

  • Shear stress produced in any material is due to relative movement of planes on each other.
  • When it comes to fluid, shear stress is produced in the fluids due to relative movement of fluid layers on one another. It is the viscosity which causes shear stress in the fluid.
  • Due to shear stress, fluid cannot be held in one place.
  • Thus, the shear stress produced in the fluid is equal to the  
ezgif 4 8b515205cb

Where μ= Dynamic Viscosity

             u= Flow Velocity

             y= Height above the boundary

  • This equation is also known as Newton’s Law of Viscosity.

Read more about Shear Strain and All important facts

Shear Rate

  • Shear rate is the rate at which one layer of fluid passes on another adjacent layer of fluid; this can find out by both using geometry and speed of the flow.
  • The viscosity of fluid mainly depends upon the shear rate of the fluid.
  • This parameter is very important while designing fluid products like syrups, sunscreen cream, body lotion, etc.

Shear Stress vs Shear Rate

  • The shear rate is defined as the rate of change of velocity of layers of fluid on one another. For all Newtonian fluids, the viscosity remains constant when there is a change in shear rate, and the shear stress is directly proportional to the shear rate. 
  • Following is a graphical representation of shear stress vs shear for a different type of fluid:
Shear Stress vs Shear Rate
Shear Stress vs Shear Rate for Newtonian Fluids

Shear Stress in Beams

  • If a cantilever beam of diameter d is twisted on its free end, if torsion of magnitude T is applied on its free end, then the shear stress produced in the beam.
  • This shear stress is represented as follows  
ezgif 4 346eadbff4
Shear Stress in Beams
Shear Stress in Beams

Shear Stress due to Bending

  • For an ideal case, shear stress does not produce due to bending, but in real condition, shear stress occurs in the bending conditions.
  • A varying bending moment along the length of the beam causes movement of one plane on another because shear stress gets produced in the beams.

Read more about Shear modulus and Modulus of rigidity

Shear Stress in Bolts

  • Bolts are mainly used to fix two different assembly bodies like joints, two different metal sheets, two different pipes of an assembly etc.
  • The bolt experiences shear load or shear force due to the presence of two different loadings acting in the different directions this causes one plane of the bolt to slip on another plane of the bolt.
  • ; This causes shear failure in joints like cotter joint, knuckle joint, etc. so, while selecting material for different mechanisms, it is essential to know its shear stress.
  • Double shear stress is calculated in bolts.
Shear Stress in Bolts
Shear Stress in Bolts

Shear Stress Steel

  • Steel is one of the most applicable metals in all types of industries. From constructions to machines, steel is used everywhere. Therefore the maximum shear stress value of steel is a significant parameter while designing.
  • It is determined using the ultimate tensile strength of the steel. Von Misses factor is used to determine maximum shear stress. It states that maximum shear stress is 0.577 times of the ultimate tensile strength.
  • In many cases, it is considered as 0.5 times of ultimate tensile strength of the steel. 

Read more about How to calculate shear strain

Shear Stress Problems

Subjective Questions

What is Shear Stress?

  Ans.: When the applied force is parallel to the surface/area of application, then the stress produced is known as shear stress. Shear stress is a component of the stress tensor in the direction parallel to the area of application.

What is complementary shear stress?

Ans.: When the shear stress is applied on a surface along the principal axis the adjacent perpendicular axis experiences the equal amount of shear stress in the opposite direction known as complementary shear stress

What are the sign conventions for shear stress? | How to decide sign of shear stress?

Ans.: Shear stress is positive if the shear force applied along the x-axis is in the right direction or clockwise.

Similarly, Shear stress is positive if the shear force applied along the y-axis is in an upward direction or it is counterclockwise.

Shear stress is negative if the shear force applied along the x-axis is in the left direction or in counterclockwise.

Similarly, Shear stress is negative if the shear force applied along the y-axis is in a downward direction or it is clockwise.

What is the sign for shear stress?

Symbol τ is used to represent shear stress. To specify the directions of applied force and direction of the application area, subscripts are used with the symbol τ as τij.

What are examples of shear?

When a piece of paper is cut with the scissor.

A bolt and nut tightly fixed with plates.

Rubbing palm on each other

Any friction leads to the production of shear.

What’s an example of shear stress?

Painting walls using colour.

Chewing food under the teeth.

In cotter and knuckle joints, cotter and knuckle experiences shear stress.

How do you solve shear stress?

Shear Stress= Force imposed parallel to the area/ Area of cross Section

ezgif 4 85c0bc9cff 1

What causes shear stress?

When force transmits from one body to another, forces parallel to the surface are experienced by the body, such kind of forces produce shear stress.

What is the difference between shear stress and shear force?

Shear force is the force applied parallel or tangential to the plane’s surface, whereas shear stress is the shear force experienced by the plane’s surface per unit area.

What is the difference between shear stress and shear rate?

When the applied force is parallel to the surface area of application, then the stress produced is known as shear stress whereas the shear rate is the rate at which one layer of fluid passes on another adjacent layer of fluid.   

What is a positive shear force?

Shear stress is positive if the shear force applied along the x-axis is in the right direction or clockwise. Similarly, Shear stress is positive if the shear force applied along the y-axis is in an upward direction or it is counterclockwise.

Positive Shear Stress
Positive and Negative Shear Stress

What is average shear stress?

Actual shear stress is never uniform; it is different for the different unit cross-sectional area. So, to calculate this shear stress, the considered shear stress is the average shear stress.

Average shear stress is always lesser than maximum shear stress for the given area of cross-section.

What is Shear Strain?

When the shear stress is applied on a surface, deformation is produced in the material. So, the ratio of deformation to the original length perpendicular to the member’s axes is known as shear strain. It is denoted by γ.

Shear Strain
Shear Strain
ezgif 4 a23b2427cb

Is shear strain in radian?

No. shear strain is the tangent value of del l and h, which is a unitless quantity.

Objective Questions:

A block of a material with a shear modulus of rigidity G = 90 KPa is bonded to two rigid horizontal plates. The lower plate is fixed, while the upper plate is subjected to a horizontal force P. knowing that the upper plate moves through 0.04 cm under the force’s action if the height of the block is 2cm, determine the average shearing strain in the material.

  1. 0.04 rad
  2. 0.02 rad
  3. 0.01 rad
  4. 0.08 rad

Solution: Option 2. Is the answer.                

ezgif 4 09055c5da6

A block of a material with a shear modulus of rigidity G = 90 KPa is bonded to two rigid horizontal plates. The lower plate is fixed, while the upper plate is subjected to a horizontal force P. knowing that the upper plate moves through 0.04 cm under the force’s action if the height of the block is 2cm, find the force P exerted on the upper plate.

  1. 180
  2. 360
  3. 720
  4. 90

Solution: Option 1. is the answer.

ezgif 4 a111d0d3cd
ezgif 4 66b0bbae6c

Find the value of shear stresses developed in the pin A for the bell crank mechanism shown in the figure? Find the safe diameter of the pin if the allowable shear stresses for the pin material is180 MPa.

  1. 3mm
  2. 4mm
  3. 4.5mm
  4. 5mm

Solution: Answer is option 4.

                   Stresses developed in pin are shear stress and bearing stress.

                   Force at B= 5*0.1/0.15= 3.33KN

ezgif 4 fc850134cf

Considering double shear at A

ezgif 4 76108afe17

The safe diameter of pin is more significant than 4.6mm.

Which of the following basic assumption is not considered while deriving torsion equation for a circular member?

  1. The material must be homogenous and isotropic.
  2. A plane perpendicular to the axis remains plane also after the torque application.
  3. Shear strain varies linearly from the central axis in a circular member when subjected to a torque.
  4. The material does not obey Hooke’s law

Solution: Option 4.

CONCLUSION 

In this article all the concepts related to shear stress are discussed in detail. It is very important to know about shear stress while designing any product.

To learn more on mechanical engineering click here!

What Is Yagi Uda Antenna: 7 Answers You Should Know

Drawing of Yagi Uda

Image Credit : Raysonho @ Open Grid Scheduler / Grid EngineYagiAntennaCC0 1.0

Points for Discussion

  • Introduction
  • Use of Yagi uda antenna
  • Elements of a typical Yagi Uda antenna
  • Yagi uda antenna construction
  • Yagi Uda Antenna Design
  • Yagi uda antenna radiation pattern
  • Few mathematical problems related to Yagi-Uda antenna

Introduction

To define a Yagi-Uda antenna, we should know the proper definition of the antenna. According to IEEE standard definitions of antennas, “An antenna is a means for radiating or receiving radio waves”.

A yagi-uda antenna is basically an array of rectilinear dipoles with a feed element and other parasitic elements. It can be described as an end-fire array which means the array is set of internally connected antennas and the total unit functions as a single antenna.

Yagi Uda Antenna

Drawing of a typical Yagi Antenna,

Image Credit- Unknown authorUnknown author, Yagi TV antenna 1954, marked as public domain, more details on Wikimedia Commons

Yagi Uda antenna is a very realistic antenna for the high-frequency domain as it operates in the high-frequency field to an ultra-high frequency domain.

Professor S. Uda and professor H. Yagi of Tohoku Imperial University, Japan, first described this type of antenna’s operation. The antenna is often interrupted as ‘Yagi Antenna’.

What is horn Antenna? Check out here!

Use of yagi uda antenna || Applications of yagi uda antenna

            Yagi antenna is one of the widely used antennae. It has been used as TV antennas at uncountable homes due to its high directivity. Many readers would recognize it just seeing the picture. It has application in amateur radios, in fields of RADARs, in satellites and RFID applications.

UHF TV Antenna 001

A modern High Frequency yagi-Uda antenna, used for television,

Image Source – Tennen-GasUHF TV Antenna 001CC BY-SA 3.0

Elements of a typical Yagi Uda antenna

As earlier said, a typical Yagi Uda antenna, is an array of small antennas and it has one element for energy feed and others are parasitic.

The most used feed element of a yagi uda antenna is a folded dipole. The radiator is specially constructed for operation of an end-fire array. Parasitic elements at the forward beam act as directors and the pieces at the rear beam act as reflectors. This completes the antenna.

The thin rods are aligned on a crossbar with their centres. There is one driven element, several parasitic elements, a reflector, and one or more directors. As the name suggests, the parasitic elements are not physically connected with the transceiver and work as passive radiators. They radiate radio waves which further affects the radiation pattern. The distance between the two rods depends on the wavelength of the signal. Typically, the distance changes from one-tenth to one-fourth of the wavelength.

The directors’ size is generally shorter than the driven element, which is also more concise than the reflector.

The gain of a yagi uda antenna depends upon the number of parasitic elements present. Increase in the number of parasitic elements increases the overall gain of the antenna. That is why there are numerous directors in a yagi-uda antenna. As the reflector has a negligible effect on the antenna gain, there is only one reflector in the antenna.

Yagi uda antenna construction

We will discuss the construction of a few parts of the yagi uda antenna. The stakes are – Driven element, Director, & the Reflector.

  • Director: It is the shortest element of the yagi uda antenna. This part is directed towards the receiving source. The length of the detectors depends upon the distance between the details and the wavelength of the signals. The gain of a yagi uda antenna has a relation with the length of the antenna. The antenna length also increases by increasing the number of directors.
  • Driven element: It is the element which has the feed point for energy. The transmitter is connected with this element through the feed point. The feed point typically lies at the centre of the component. The length of the part is half of the wavelength.
  • Reflectors: It is a single unit and constructed at the end of the antenna array just after the driven element. It has the highest length among the parasitic elements. The spacing of reflector depends on the wavelength, beamwidth and gain of the yagi uda antenna. The resonant frequency of reflector is generally lower.

How transmission lines are related with antennas? To know – click here!

Working of yagi uda antenna

Let us draw some attention towards the operation and working of a yagi uda antenna. Assume a typical yagi uda antenna with a reflector, with a driven element and a single director.

As discussed earlier, the driving element’s length is half of the dipole, and it is connected with electrical energy directly. It supplies power throughout the antenna as it has the feed point, and all other parasitic elements are internally associated with this element.

Now, assume the parasitic elements (both the reflectors and directors) as a general dipole element of a measurable diameter and fed at the middle via a short circuit. Transmission line theory says that a short circuit is enabled to reflect power at 180 degrees.

330px Yagi 3 element.svg

Parts of a typical yagi-uda antenna,

A – Driven Element, R – Reflector, D – Director,

Image Credit – SankeytmYagi 3 elementCC BY-SA 3.0

Thus, the operation can be designed as the mixing up of a power receiver dipole element that receives the power and sends to the matched load and a power transmitter dipole element that transmits the power to the array of the antenna.

Now, at an instant, if the received and sent power are in 180 degrees out of phase with each other, then the result will be zero voltage. That signifies the short circuit of the diode at the feed point. That is why the radiated power is in 180 degrees phase out with the incident waves.

The parasitic elements in the antenna are shorter than ½λ. The reflector is longer than ½λ, and it generally lags the phase of open-circuit voltage. The incoming signal generates the voltage. The director is also shorter than ½λ. It lags the voltage that of current.

Yagi Uda antenna design

Unlike the horn antenna, there are no hard and fast rules to design a yagi-uda antenna. There are some critical physical parameters which resist doing so. Some of the parameters are as follow –

  • ‘Length of element and distance between them.’
  • The measurement of the rods or the diameter of the rods.
  • Some critical parameters like – Gain and input resistance.

Though, there are some methods for analysis and calculation to find out the desired results. For an n-element yagi uda antenna, there are 2n-1 numbers of parameters to consider.

The analysis for current distribution is done by solving the ‘Hallen’s integral equation’. The assumption of a classical standing wave and condition of other conductors are also taken into account. The analysis method is complicated and requires accurate results though some vital approximations are necessary to complete it.

The designed antennas go through trial-and-error methods to modify further. Sometimes, the antenna starts with a design and ends up with another after certain modifications in the process. Nowadays, computer simulation helps designers/ engineers to check the result.

Yagi Uda antenna radiation pattern

Radiation Pattern is the angular dependence of the strength of the radio waves from any electromagnetic source. The below image shows the radiation pattern of a yagi uda antenna.

Yagi antenna animation 16 frame 1.6s
Yagi uda antenna radiation pattern, Image By – ChetvornoYagi antenna animation 16 frame 1.6sCC0 1.0

Advantages yagi uda Antenna || Disadvantages of yagi uda antenna

            Yagi uda antenna has both its advantages and disadvantages. But there is no doubt that this antenna has made some drastic changes in the field of commercial antennas. It has the highest ever popularity as TV antennas because of its large bandwidth. Let us discuss some of its advantages.

Advantages of yagi uda antenna

  • Yagi uda antenna has a decent gain of 7dB, which is sufficient for its applications.
  • Yagi uda antenna array is direction type of antenna.
  • This type of antennas is suitable for applications in high frequency to the ultra-high frequency range.
  • These antennas have adjustable from to ack ratio.

Let us discuss some drawbacks of yagi uda antenna.

Disadvantages of yagi uda antenna

  • Though the applications of yagi uda antennas are suitable for the antenna’s gain, the gain is not very high compared to any other types of antenna.
  • The designing has a requirement of a large number of elements.
  • Any damage to the parasitic elements leads to the dysfunctionality of the whole antenna.
  • The size is quite large, that is why nowadays the antennas are not used by peoples.

Few mathematical problems related to Yagi Uda Antenna

1. Design a yagi uda antenna with the following specifications. Directivity: Relative to ½λ dipole and situated at the same level. Magnitude: 9.2 dB. f0 = 50.1 MHz. The desired diameter of the parasitic rods: 2.54 cm. The desired diameter of the metal supporting boom: 5.1 cm. Find out the spacings between elements, lengths and length of the entire array.

Solution:

            The operating frequency is given as 50.1 MHz. The wavelength comes as λ = 5.988m.

The desired diameter of the parasitic rods is given as d = 2.54 cm.

Therefore, d /λ = 2.54/598.8

Or, d /λ = 4.24 x 10-3 

The desired diameter of the metal supporting boom is given as D = 5.1cm.

Therefore, D /λ = 5.1 / 598.8

Or, D /λ = 8.52 x 10-3

            We need to use a chart that gives us ‘optimized uncompressed lengths of parasitic elements of a yagi-uda antenna’. Using this chart, we can understand that the desired antenna array would have a total of five elements (one driven element, one reflector and three directors).

The second column of the chart gives us the optimum uncompressed length for the value of d/λ = 0.0085.

l1 = 0.482λ

l3 = 0.428λ

l4 = 0.424λ

l5 = 0.428λ

The overall antenna length will be L = (0.6 + 0.2) λ = 0.8λ. The spacing or the distance between the directors parasitic will be 0.2λ and the spacing of the reflector will be same that is 0.2λ.

What Is Poisson’s Ratio: 9 Facts You Should Know

e8

When a deformable material is stretched in a particular direction, its length increases in that direction, and thickness reduces in the lateral one. Similarly, the material is compressed in a specific direction and, its length decreases in that direction, and thickness increases in the lateral one. Poisson’s ratio is a parameter that relates these deformations, which is useful in material selection and application.

Poisson’s Ratio Definition | Poisson’s Ratio Equation

When we apply tensile stress on the material, there is elongation in the direction of applied force and shrinkage in the transverse/lateral movement. Thus the strain gets produced in both directions. The ratio of strain produced in the transverse direction to the strain produced in the direction of tensile stress application is known as Poisson’s ratio.

Its symbol is ʋ or μ.

The ratio obtained has a negative sign, as the ratio obtained is always negative.

Thus,

        Poisson’s Ratio= Transverse Strain/ axial Strain

                           ʋ= -(εxy)

Poisson's Ratio: formula
Poisson's Ratio: Figure
Figure : Lateral Strain

Similarly, if compressive stress is applied to the material, there is shrinkage in the direction of applied force and thickening in the transverse/ lateral direction. Thus, the strain gets produced in both directions. The ratio of strain produced in the transverse direction to the strain produced in the direction of compressive stress application is also known as Poisson’s ratio.

Generally, it ranges from 0 to 0.5 for engineering materials. Its value increases under tensile stress and decreases under compressive stress.

For more details click here!

Poisson’s Ratio of Steel

  • The value of Poisson’s ratio for steel ranges from 0.25 to 0.33.
  • The average value of Poisson’s ratio for steel 0.28.
  • It depends on the steel type used.

Following is the list of Poisson’s ratio for different steels

Steel TypePoisson’s Ratio
High Carbon Steel0.295
Mild Steel0.303
Cast Steel0.265
Cold Rolled Steel0.287
Stainless Steel 18-80.305( 0.30-0.31)

Poisson’s Ratio of Aluminum

  • The value of Poisson’s ratio for aluminum ranges from 0.33 to 0.34.
  • The average value of Poisson’s ratio for aluminum is 0.33 and for aluminum alloy 0.32.
  • It depends on the type of aluminum or aluminum alloy used.

Following is the list of Poisson’s ratio for different aluminum

Aluminum TypePoisson’s Ratio
Aluminum Bronze0.30
Rolled Aluminum0.337/0.339
Rolled Pure Aluminum0.327

 Poisson’s Ratio of Concrete

  • The value of Poisson’s ratio for concrete ranges from 0.15 to 0.25.
  • Its general value is taken as 0.2.
  • It depends on the type of concrete (wet, dry, saturated) and loading conditions.
  • Its value for high strength concrete is 0.1, and for low strength concrete, it is o.2.

Poisson’s Ratio of Copper

  • The value of Poisson’s ratio ranges from 0.34 to 0.35.
  • Its general value is taken as 0.355.
  • It depends on the type of copper or copper alloy used.

Following is the list of Poisson’s ratio for different copper

Copper TypePoisson’s Ratio
Normal Brass0.34
Brass, 70-30              0.331
Brass, cast     0.357
Bronze0.34

Poisson’s Ratio of Rubber

  • The value of Poisson’s ratio for rubber is from 0.48 to 0.50.
  • For most of the rubbers, it is equal to 0.5.
  • Its value for natural rubber is 0.5.
  • It has the highest value of Poisson’s Ratio. 

Poisson’s Ratio of Plastic

  • The Poisson’s ratio of plastics generally increases with time, strain, and temperature and decreases with strain rate.
  • Following is the list of Poisson’s ratio for different plastics
Plastic TypePoisson’s Ratio
PAMS0.32
PPMS0.34
PS0.35
PVC0.40

Poisson’s Ratio and Young’s Modulus

The materials for which elastic behavior does not vary with the crystallographic direction are known as elastically isotropic materials. Using Poisson’s ratio of the material, we can obtain a relation between Modulus of Rigidity and Modulus of Elasticity for isotropic materials as follows.

                                  Y= 2*G*(1+ʋ)

Where, Y= Modulus of Elasticity

             G= Modulus of Rigidity

             ʋ= Poisson’s Ratio

Questions and Answers

What is meant by Poisson’s ratio?

 When we apply tensile stress on the material, there is elongation in the direction of applied force and shrinkage in the transverse/lateral direction. Thus the strain gets produced in both directions. The ratio of strain produced in the transverse direction to the strain produced in the direction of tensile stress application is known as Poisson’s ratio.

Poisson's Ratio
Figure : Lateral Strain

What does a Poisson ratio of 0.5 mean?

Poisson’s ratio of precisely 0.5 means the material is perfectly incompressible isotropic material deformed elastically at small strains.

How is Poisson’s ratio calculated?

        Poisson’s Ratio= Transverse Strain/ axial Strain

                           ʋ=-εx/εy

e8 1
7 2
Figure : Lateral Strain

What is the Poisson’s ratio for steel?

The value of Poisson’s ratio for steel ranges between 0.25 to 0.33.

The average value of Poisson’s ratio for steel 0.28.

What is Poisson’s ratio for aluminum?

The value of Poisson’s ratio for aluminum ranges between 0.33 to 0.34.

The average value of Poisson’s ratio for aluminum is 0.33 and for aluminum alloy 0.32.

What is Poisson’s ratio for concrete?

The value of Poisson’s ratio for concrete ranges between 0.15 to 0.25.

Its general value is taken as 0.2.

It depends on the type of concrete (wet, dry, saturated) and loading conditions.

Its value for high strength concrete is 0.1, and for low strength concrete, it is 0.2.

What is the relation between Poisson’s Ratio and Young’s Modulus of Elasticity?

                                  Y= 2*G*(1+ʋ)

Where, Y= Modulus of Elasticity

             G= Modulus of Rigidity

             ʋ= Poisson’s Ratio

Which parameters affect the Poisson’s Ratio of Polymers?

The Poisson’s ratio of polymeric materials like plastic generally increases with time, strain, and temperature and decreases with strain rate.

What if Poisson’s ratio is zero?

If the Poisson’s ratio is zero, the material is not deformable; hence, it is a rigid body.

Which material has the highest Poisson’s ratio?

Rubber has the highest Poisson’s Ratio, almost equal to 0.5.

Why is Poisson’s ratio always positive?

Poisson’s ratio is the negative of the ratio of lateral strain to axial strain. The ratio of lateral strain to axial strain is always negative because elongation causes contraction in diameter, which ultimately makes the ratio negative .similarly, compression causes elongation in diameter, which makes the ratio negative.

Is Poisson’s ratio constant?

For the stresses in the elastic range, Poisson’s ratio is almost constant.

Does Poisson’s ratio dependent on temperature?

Yes. With the increasing temperature, Poisson’s ratio decreases.

Objective Questions

Tensile stress is applied along the longitudinal axis of a cylindrical brass rod with a diameter of 10mm. Determine the magnitude of the strain produced in the transverse direction where the load is required to produce a 2.5 *10-3 change in diameter if the deformation is entirely elastic. Poisson’s ratio of brass is 0.34.

Objective Question :1
  1. 3.5*10-3
  2. 5.5*10-3
  3. 7.35*10-3
  4. 1.0*10-3

Solution: Answer is option 3.

 { \\epsilon }_{ x }=\\frac { \\triangle d }{ { d }_{ o } } =\\frac { -2.5\\times { 10 }^{ -3 } }{ 10 } =-2.5\\times { 10 }^{ -4 }

{ \\epsilon }_{ z }=-\\frac { { \\epsilon }_{ x } }{ \\upsilon } =-\\frac { -2.5\\times { 10 }^{ -4 } }{ 0.34 } =7.35\\times { 10 }^{ -4 }

A wire of length 2 m is loaded, and an elongation of 2mm is produced. If the wire’s diameter is 5 mm, find the change in the diameter of the wire when elongated. Poisson’s ratio of the wire is  0.35

Solution: L= 2m

                 Del L= 2mm

                 D= 1mm

                 ʋ= 0.24

                Longitudinal Strain= 2*10-3/2=10-3

                Lateral Strain= Poisson’s Ratio*Longitudinal Strain

                                        = 0.35*10-3

                Lateral Strain= Change in diameter/ Original Diameter=0.35*10-3

                                                                             Change in Diameter=0.35*10-3*5*10-3

                                                                                                                = 1.75*10-6

                                                                                                                =1.75*10-7 

                 Thus, the Change in diameter is 1.75*10-7mm.

A wire of steel having a cross-sectional area of 2 mm2 is stretched by 20 N. Find the lateral strain produced in the wire. Young’s Modulus for steel is 2*1011N/m2, and Poisson’s ratio is 0.311.

Solution: A= 2mm2= 2*10-6mm2

                 F= 20N

                                                 Y= Longitudinal Stress/ Longitudinal Strain

                                                   =F/ (A*Longitudinal Strain)

                 Longitudinal Strain= F/(Y*A)

                                                   =20/ (1*10-6*2*1011) = 10-4

              Poisson’s Ratio= Lateral Strain/ Longitudinal Strain

              Lateral Strain= Poisson’s Ratio*Longitudinal Strain

                                    = 0.311*10-4

              Lateral Strain=0.311*10-4

Conclusion

In this articles, all the important concepts related to Poisson’s Ratio are discussed in detailed . Numerical and subjective type of questions are added for practice.

To learn more on strength of material Click Here!

Heat Transfer Enhancement In Nanofluid: 9 Important Facts

graph1 300x248 1

Nanofluids have emerged as a promising solution for enhancing heat transfer in various applications. By incorporating nanoparticles into conventional heat transfer fluids, nanofluids exhibit improved thermal properties that can significantly enhance heat transfer efficiency. In this section, we will explore the definition and composition of nanofluids, as well as their application in heat transfer enhancement.

Definition and Composition of Nanofluids

Nanofluids can be defined as suspensions of nanoscale particles in a base fluid, typically water or oil. These nanoparticles, which are usually metallic or non-metallic, are dispersed uniformly in the base fluid, creating a stable colloidal mixture. The size of the nanoparticles used in nanofluids typically ranges from 1 to 100 nanometers.

The composition of nanofluids plays a crucial role in determining their heat transfer properties. The choice of nanoparticles and base fluid depends on the specific application requirements. Metallic nanoparticles, such as copper, aluminum, and silver, are commonly used due to their high thermal conductivity. Non-metallic nanoparticles, such as carbon nanotubes and graphene, are also gaining attention for their unique properties.

To ensure the stability of nanofluids, various techniques are employed to prevent particle agglomeration. Surface modification of nanoparticles, such as coating them with surfactants or polymers, helps to maintain the stability and prevent sedimentation. Additionally, ultrasonication and magnetic stirring are used during the synthesis process to disperse the nanoparticles evenly in the base fluid.

Application of Nanofluids in Heat Transfer Enhancement

The use of nanofluids in heat transfer applications has gained significant interest due to their ability to enhance thermal conductivity and convective heat transfer. The incorporation of nanoparticles into the base fluid increases the effective thermal conductivity of the nanofluid, resulting in improved heat transfer rates.

Nanofluids find applications in various heat transfer systems, including heat exchangers, electronics cooling, and solar thermal systems. In heat exchangers, nanofluids can enhance the overall heat transfer coefficient, leading to improved system performance. The increased heat transfer efficiency of nanofluids allows for smaller heat exchanger designs, reducing space and cost requirements.

In electronics cooling, nanofluids offer a solution to dissipate heat generated by electronic devices more effectively. By using nanofluids as coolants, the heat transfer rate from the electronic components to the cooling system can be significantly improved, ensuring optimal device performance and reliability.

Furthermore, nanofluids have shown promise in solar thermal systems, where they can enhance the absorption and transfer of solar energy. The improved heat transfer properties of nanofluids enable more efficient conversion of solar radiation into usable heat, making them a potential solution for sustainable energy applications.

Heat Transfer Enhancement in Nanofluids

Overview of Heat Transfer Enhancement in Nanofluids

graph1

Nanofluids, a combination of base fluids and nanoparticles, have gained significant attention in recent years due to their ability to enhance heat transfer. These nanofluids exhibit improved thermal properties compared to traditional fluids, making them a promising solution for various heat transfer applications. In this section, we will explore the concept of heat transfer enhancement in nanofluids and delve into the underlying mechanisms that contribute to their superior performance.

Nanofluids are engineered by dispersing metallic or non-metallic nanoparticles, typically in the range of 1-100 nanometers, into a base fluid such as water, oil, or ethylene glycol. The addition of nanoparticles alters the thermal conductivity, viscosity, and convective heat transfer characteristics of the base fluid, leading to enhanced heat transfer rates.

One of the key factors that contribute to the improved heat transfer in nanofluids is the significantly higher thermal conductivity of nanoparticles compared to the base fluid. The presence of nanoparticles in the fluid creates a conductive network that facilitates the transfer of heat. This increased thermal conductivity allows for more efficient heat dissipation, resulting in enhanced heat transfer rates.

Importance of Thermal Conductivity in Nanofluids

Thermal conductivity plays a crucial role in determining the heat transfer performance of nanofluids. The ability of a material to conduct heat is quantified by its thermal conductivity coefficient. In the case of nanofluids, the thermal conductivity is significantly enhanced due to the presence of nanoparticles.

The high thermal conductivity of nanoparticles allows for better heat conduction within the nanofluid, enabling faster heat transfer. This property is particularly beneficial in applications where heat dissipation is critical, such as heat exchangers or electronic cooling systems. By utilizing nanofluids with enhanced thermal conductivity, the overall efficiency of these systems can be greatly improved.

Moreover, the increased thermal conductivity of nanofluids also leads to a higher heat transfer coefficient. The heat transfer coefficient represents the rate at which heat is transferred between a solid surface and a fluid. In the case of nanofluids, the higher thermal conductivity results in a larger heat transfer coefficient, indicating a more efficient heat transfer process.

In addition to thermal conductivity, the convective heat transfer characteristics of nanofluids are also influenced by the presence of nanoparticles. The nanoparticles alter the fluid dynamics within the nanofluid, promoting better heat transfer through convection. This enhanced convective heat transfer further contributes to the overall heat transfer enhancement in nanofluids.

Methods to Increase Heat Transfer

Heat transfer is a crucial process in various industrial applications, ranging from cooling electronic devices to optimizing the efficiency of power plants. Enhancing heat transfer is essential to improve the overall performance and effectiveness of these systems. In recent years, researchers have been exploring innovative methods to increase heat transfer, including the use of nanofluids. Nanofluids, which are a combination of nanoparticles and base fluids, have shown great potential in enhancing heat transfer due to their unique thermal properties. In this section, we will explore different ways to enhance heat transfer and delve into the fascinating world of nanofluid technology.

Before we delve into the ways to enhance heat transfer, let’s first understand the fundamental equation that governs heat transfer. The heat transfer equation, also known as Fourier’s law, describes the rate at which heat is transferred through a material. It states that the heat transfer rate is directly proportional to the temperature gradient and the thermal conductivity of the material, and inversely proportional to the thickness of the material. Mathematically, it can be represented as:

q = -k * A * (dT/dx)

Where:
– q is the heat transfer rate
– k is the thermal conductivity of the material
– A is the cross-sectional area through which heat is transferred
– dT/dx is the temperature gradient across the material

Understanding this equation is crucial as it forms the basis for exploring methods to enhance heat transfer.

Ways to Enhance Heat Transfer

Now that we have a basic understanding of the heat transfer equation, let’s explore some ways to enhance heat transfer. These methods can be broadly categorized into two main approaches: improving thermal conductivity and optimizing convective heat transfer.

Improving Thermal Conductivity

One way to enhance heat transfer is by improving the thermal conductivity of the working fluid. Thermal conductivity refers to the ability of a material to conduct heat. By incorporating high thermal conductivity nanomaterials, such as metallic or carbon-based nanoparticles, into the base fluid, the overall thermal conductivity of the nanofluid can be significantly enhanced. These nanoparticles, due to their small size and large surface area, facilitate efficient heat transfer by increasing the number of heat transfer pathways within the fluid.

Optimizing Convective Heat Transfer

Convective heat transfer, which occurs when a fluid flows over a solid surface, is another area where heat transfer enhancement can be achieved. By using nanofluids, researchers have observed improvements in convective heat transfer due to the unique properties of nanoparticles. The presence of nanoparticles in the fluid alters its flow behavior, leading to enhanced heat transfer. The nanoparticles act as disruptors, breaking up the thermal boundary layer near the solid surface and promoting better heat transfer between the fluid and the surface.

To optimize convective heat transfer, researchers have explored various parameters, such as nanoparticle concentration, particle size, and flow velocity. By carefully tuning these parameters, it is possible to achieve significant improvements in heat transfer performance. Additionally, the use of advanced heat exchangers and fluid dynamics techniques can further enhance convective heat transfer in nanofluids.

Comparison of Various Nanofluids

Overview of Nanofluid Thermal Conductivity Dependence on Metallic Particle Properties

Nanofluids, which are colloidal suspensions of nanoparticles in a base fluid, have gained significant attention in recent years due to their potential for enhancing heat transfer in various applications. Metallic nanoparticles, such as copper, silver, and aluminum, are commonly used in nanofluids due to their high thermal conductivity and stability.

The thermal conductivity of nanofluids is influenced by several factors, including the properties of the metallic nanoparticles. The size, shape, and concentration of the nanoparticles play a crucial role in determining the thermal conductivity enhancement of the nanofluid.

Size: The size of the nanoparticles affects the thermal conductivity enhancement of the nanofluid. Smaller nanoparticles have a larger surface area-to-volume ratio, which promotes better heat transfer. As the particle size decreases, the phonon scattering at the nanoparticle-fluid interface increases, leading to enhanced thermal conductivity.

Shape: The shape of the nanoparticles also impacts the thermal conductivity of the nanofluid. Nanoparticles with a higher aspect ratio, such as nanorods or nanowires, exhibit better thermal conductivity enhancement compared to spherical nanoparticles. The elongated shape provides a larger contact area, facilitating efficient heat transfer.

Concentration: The concentration of metallic nanoparticles in the nanofluid affects the thermal conductivity enhancement. As the nanoparticle concentration increases, the interparticle interactions and clustering can occur, leading to a decrease in thermal conductivity. However, at lower concentrations, the nanoparticles disperse more uniformly, resulting in enhanced thermal conductivity.

Comparison of Different Nanofluids for Heat Transfer Enhancement

Numerous studies have been conducted to compare the heat transfer enhancement capabilities of different nanofluids. These studies have focused on various factors, including the type of nanoparticles, base fluid, and experimental conditions. Let’s take a look at some of the key findings:

  1. Metallic Nanoparticles: Nanofluids containing metallic nanoparticles, such as copper, silver, and aluminum, have shown significant heat transfer enhancement compared to pure base fluids. The high thermal conductivity of these metallic nanoparticles facilitates efficient heat transfer, making them suitable for applications in heat exchangers and cooling systems.

  2. Carbon-Based Nanoparticles: Carbon-based nanoparticles, such as graphene and carbon nanotubes, have also demonstrated excellent heat transfer enhancement properties. These nanoparticles have high thermal conductivity and unique structural properties, enabling efficient heat dissipation. However, challenges related to dispersion and stability need to be addressed for practical applications.

  3. Oxide Nanoparticles: Nanofluids containing oxide nanoparticles, such as alumina and titania, have been extensively studied for heat transfer enhancement. These nanoparticles offer good stability and have the potential to enhance convective heat transfer. However, their lower thermal conductivity compared to metallic nanoparticles limits their overall heat transfer enhancement capabilities.

  4. Hybrid Nanofluids: Hybrid nanofluids, which combine different types of nanoparticles, have also been investigated for heat transfer enhancement. These nanofluids aim to leverage the unique properties of multiple nanoparticles to achieve enhanced heat transfer performance. However, further research is needed to optimize the nanoparticle combination and concentration for maximum heat transfer enhancement.

Applications of Nanofluids in Heat Transfer

Nanofluids, which are suspensions of nanoparticles in a base fluid, have gained significant attention in recent years due to their remarkable thermal properties. These unique fluids have found numerous applications in various heat transfer systems, ranging from electronic cooling to solar thermal devices. Let’s explore some of the key applications of nanofluids in heat transfer.

Use of Nanofluids in Electronic Cooling

Electronic devices generate a substantial amount of heat during operation, which can lead to performance degradation and even failure if not properly managed. Nanofluids offer a promising solution for efficient electronic cooling. Two commonly used techniques for electronic cooling are the vapor chamber and jet impingement methods.

Vapor Chamber

Vapor chambers are heat pipes that utilize the evaporation and condensation of a working fluid to transfer heat. By incorporating nanofluids as the working fluid, the heat transfer performance can be significantly enhanced. The high thermal conductivity of nanoparticles improves the overall heat transfer rate, allowing for more efficient cooling of electronic components.

Jet Impingement

Jet impingement cooling involves directing a high-velocity fluid jet onto the surface of a heated object. Nanofluids can be employed in this process to enhance convective heat transfer. The presence of nanoparticles in the fluid increases the heat transfer coefficient, resulting in improved cooling efficiency. This makes nanofluids an excellent choice for cooling high-power electronic devices.

Application of Nanofluids in Radiators for Engine Cooling

Efficient cooling is crucial for the proper functioning of internal combustion engines. Traditional coolants, such as water or ethylene glycol, can be enhanced by adding nanoparticles to form nanofluids. These nanofluids exhibit superior thermal conductivity compared to conventional coolants, leading to improved heat dissipation from the engine.

By utilizing nanofluids in radiators, the heat transfer rate can be significantly increased. This translates to better engine performance, reduced fuel consumption, and lower emissions. Moreover, nanofluids offer enhanced stability and reduced corrosion, making them an attractive option for engine cooling applications.

Utilization of Nanofluids in Solar Thermal Devices

Solar thermal devices, such as parabolic solar collectors, harness the energy from the sun to generate heat. Nanofluids can play a vital role in enhancing the efficiency of these devices. By incorporating nanoparticles into the heat transfer fluid, the thermal conductivity is improved, resulting in more effective heat absorption and transfer.

The use of nanofluids in solar thermal devices allows for higher operating temperatures and increased energy conversion efficiency. This, in turn, leads to improved performance and reduced costs in solar power generation. Nanofluids have the potential to revolutionize the field of solar energy by maximizing the utilization of available sunlight.

Nanofluid Application in Transformer Cooling

Transformers are essential components in electrical power systems, and efficient cooling is crucial to ensure their reliable operation. Nanofluids offer a promising solution for transformer cooling due to their excellent thermal properties. By using nanofluids as the cooling medium, the heat transfer rate can be significantly enhanced.

Nanofluids provide improved thermal conductivity and heat transfer coefficients compared to traditional cooling fluids. This allows for more efficient heat dissipation from the transformer, reducing the risk of overheating and extending its lifespan. The application of nanofluids in transformer cooling systems can lead to enhanced reliability and reduced maintenance costs.

Other Applications of Nanofluids in Cooling and Heat Transfer Systems

In addition to the aforementioned applications, nanofluids have found use in various other cooling and heat transfer systems. Some notable examples include:

  • Heat exchangers: Nanofluids can be employed in heat exchangers to enhance heat transfer efficiency and reduce energy consumption.
  • Fluid dynamics: Nanofluids have been studied extensively to understand their flow behavior and optimize their performance in different applications.
  • Nanotechnology: The field of nanotechnology has benefited greatly from the development of nanofluids, as they offer unique opportunities for heat transfer enhancement at the nanoscale.
  • Nanofluid synthesis: Researchers continue to explore new methods for synthesizing nanofluids with improved stability and enhanced thermal properties.
  • Nanofluid properties: The study of nanofluid properties, such as viscosity, density, and thermal conductivity, plays a crucial role in optimizing their performance in various heat transfer systems.

Feasibility and Future Scope of Nanofluids

Nanofluids, a suspension of nanoparticles in a base fluid, have gained significant attention in recent years due to their potential for enhancing heat transfer in various applications. In this section, we will explore the feasibility of nanofluids as thermal fluids, discuss their importance in increasing equipment efficiency, and highlight the future prospects and research opportunities in this exciting field.

Feasibility of Nanofluids as Thermal Fluids

Nanofluids offer several advantages over traditional heat transfer fluids. The addition of nanoparticles to the base fluid enhances its thermal conductivity, which is crucial for efficient heat transfer. The high surface area-to-volume ratio of nanoparticles allows for better heat dissipation, leading to improved thermal performance.

Moreover, nanofluids exhibit unique properties at the nanoscale, such as enhanced convective heat transfer and altered fluid dynamics. These properties make them suitable for a wide range of applications, including heat exchangers, cooling systems, and thermal management in electronic devices.

To ensure the feasibility of nanofluids, researchers have focused on studying their stability, flow characteristics, and thermal properties. Stability is a critical factor as nanoparticles tend to agglomerate, affecting the overall performance of the nanofluid. By employing suitable surfactants and dispersants, scientists have made significant progress in stabilizing nanofluids and preventing particle aggregation.

Importance of Nanofluids in Increasing Equipment Efficiency

The use of nanofluids can significantly enhance the efficiency of various equipment and systems. By improving heat transfer, nanofluids can reduce the energy consumption of heat exchangers, leading to cost savings and environmental benefits. The enhanced heat transfer coefficient and heat transfer rate of nanofluids ensure that heat is efficiently transferred between the solid surface and the fluid.

Additionally, the unique properties of nanofluids, such as their ability to alter fluid dynamics, enable the design of more compact and efficient heat exchangers. This, in turn, leads to space savings and increased performance in a wide range of applications, including automotive cooling systems, power plants, and electronic devices.

Future Prospects and Research Opportunities in Nanofluids

The field of nanofluids holds immense potential for future advancements and research opportunities. As nanotechnology continues to evolve, researchers are exploring novel nanomaterials and nanoparticles that can further enhance the thermal properties of nanofluids. By tailoring the size, shape, and composition of nanoparticles, scientists can optimize their heat transfer capabilities for specific applications.

Moreover, understanding the underlying heat transfer mechanisms in nanofluids is crucial for their successful implementation. Ongoing research aims to elucidate the fundamental mechanisms responsible for the enhanced heat transfer observed in nanofluids. This knowledge will enable the development of predictive models and simulations, facilitating the design and optimization of nanofluid-based systems.

Furthermore, the application of nanofluids extends beyond heat transfer enhancement. Researchers are exploring the use of nanofluids in areas such as energy storage, solar thermal systems, and biomedical applications. The versatility of nanofluids opens up new avenues for innovation and cross-disciplinary collaborations.

Frequently Asked Questions

1. How does nano heat transfer differ from traditional heat transfer?

Nano heat transfer refers to the study and application of heat transfer at the nanoscale, involving the transfer of heat between objects or systems at the nanometer level. Traditional heat transfer, on the other hand, deals with heat transfer at macroscopic scales. Nano heat transfer takes into account unique phenomena and properties that arise at the nanoscale, such as quantum effects and surface interactions.

2. What is heat transfer enhancement using nanofluids?

Heat transfer enhancement using nanofluids involves the incorporation of nanoparticles into conventional heat transfer fluids to improve their thermal properties. By adding nanoparticles, such as metal or oxide particles, to the base fluid, the thermal conductivity and convective heat transfer characteristics of the fluid can be enhanced, leading to improved heat transfer rates in various applications.

3. How can heat transfer be increased using nanofluids?

Heat transfer can be increased using nanofluids by exploiting the enhanced thermal conductivity and convective heat transfer properties of the nanoparticles suspended in the fluid. The nanoparticles facilitate better heat transfer by increasing the effective thermal conductivity of the fluid and promoting convective heat transfer through improved fluid dynamics. This results in higher heat transfer rates compared to conventional fluids.

4. What are the techniques for heat transfer enhancement using nanofluids?

There are several techniques for heat transfer enhancement using nanofluids, including altering the nanoparticle concentration, controlling the particle size and shape, optimizing the fluid flow conditions, and utilizing surface modifications to enhance the interaction between the nanoparticles and the fluid. These techniques aim to maximize the thermal properties and convective heat transfer characteristics of the nanofluid, leading to improved heat transfer rates.

5. How does nanotechnology contribute to heat transfer enhancement?

Nanotechnology plays a crucial role in heat transfer enhancement by enabling the synthesis and manipulation of nanomaterials and nanoparticles with unique thermal properties. Through nanotechnology, researchers can design and engineer nanofluids with enhanced thermal conductivity and convective heat transfer characteristics, thereby improving heat transfer rates in various applications, such as heat exchangers and thermal management systems.

6. What is the role of nanofluid flow in heat transfer enhancement?

Nanofluid flow plays a significant role in heat transfer enhancement as it affects the convective heat transfer characteristics of the fluid. By optimizing the flow conditions, such as flow rate, velocity, and turbulence, the interaction between the nanoparticles and the fluid can be maximized, leading to improved heat transfer rates. Proper understanding and control of nanofluid flow dynamics are essential for effective heat transfer enhancement.

7. How does nanofluid stability impact heat transfer enhancement?

Nanofluid stability is crucial for heat transfer enhancement as it ensures the uniform dispersion and suspension of nanoparticles in the base fluid. Stable nanofluids prevent particle agglomeration and sedimentation, which can hinder the convective heat transfer process. By maintaining nanofluid stability, the nanoparticles can effectively enhance the thermal conductivity and convective heat transfer properties of the fluid, leading to improved heat transfer rates.

8. What are the heat transfer mechanisms in nanofluids?

The heat transfer mechanisms in nanofluids involve three main processes: conduction, convection, and radiation. Conduction refers to the transfer of heat through direct particle-to-particle contact, while convection involves the transfer of heat through the movement of the nanofluid. Radiation, on the other hand, occurs when heat is transferred through electromagnetic waves. The combination of these mechanisms contributes to the overall heat transfer enhancement in nanofluids.

9. What are the applications of nanofluids in heat transfer?

Nanofluids find various applications in heat transfer, including heat exchangers, electronics cooling, solar thermal systems, and automotive cooling systems. The enhanced thermal properties and convective heat transfer characteristics of nanofluids make them suitable for improving heat transfer rates in these applications. Nanofluids offer potential benefits in terms of increased energy efficiency and improved thermal management.

10. How are nanofluids synthesized for heat transfer enhancement?

Nanofluids can be synthesized through various methods, including one-step and two-step processes. One-step synthesis involves directly dispersing nanoparticles into the base fluid, while two-step synthesis involves the separate synthesis of nanoparticles followed by their dispersion into the fluid. The choice of synthesis method depends on factors such as nanoparticle material, desired concentration, and stability requirements.

What Is Horn Antenna: 9 Important Concepts

ATM Horn Antennas 300x228 1

Image Credit: Schwarzbeck Mess-Elektronik, Schwarzbeck BBHA 9120 DCC BY-SA 3.0

Points for Discussion: Horn Antenna

  • Introduction
  • Use of horn antenna
  • Elements of a horn antenna and Types of horn antenna
  • Horn antenna design
  • Directivity of horn antenna
  • Horn antenna radiation pattern
  • Horn antenna gain
  • Horn antenna beamwidth
  • Few mathematical problems related to Horn Antenna

Introduction

To define a horn antenna, we should know the proper definition of the antenna. According to IEEE standard definitions of antennas,

“An antenna is a means for radiating or receiving radio waves”.

Horn antenna is the most popular type of Aperture antenna. Aperture antennas are specially designed for microwave frequencies. These types of aperture antennas are widely used and most unadorned other than any kinds.

Though horn antenna usage was started back in the 1800s, the rapid application was created in the 1930s. These antennas had also undergone drastic modification during this time. Numerous thesis and research were done to describe the horn-antenna’s design, find out the radiation pattern of horn-antenna, and applications in different sectors. The applications in microwave and waveguide transmission domain made horns antenna famous. That is why horn- antennas are often interpreted as a microwave horn-antenna.

What is Transmission Line? How it is related to antenna? Know here!

Use of Horn Antenna

Horn-antennas have found impactful applications as feed elements for hefty radio astronomy, satellite tracking, communication dishes, and many other places. It is used as a feed for reflector and lenses and also used in phased arrays. These antennas are preferred over different types of aperture antennas, because of its fair and straightforward design, better gain, versatility, and overall performance.

Elements of a horn antenna

Horn antenna is a resonating pipe of various designs which can be shaped for making a larger opening. The overall performance of the antenna is affected by the direction, taper’s amount, directivity.

Types of horn antenna

Horn-antennas have different forms for operations. They are –

·       Sectoral Horn Antenna

  • E-Plane
  • H-Plane

·       Pyramidal Horn Antenna

ATM Horn Antennas
A typical pyramidal horn -antenna, Credit – Tactron ElektronikATM Horn AntennasCC BY-SA 3.0

·       Conical Horn Antenna

BocinaLenteDielectrica
Conical Horn -Antenna and its radiation pattern; Image Credit – Mª Luisa BelloBocinaLenteDieléctricaCC BY-SA 4.0

·       Corrugated horn antenna

640px LNB 2
Corrugated horn- antenna; Image Credit: Laurent06LNB 2CC BY-SA 3.0

·       Diagonal horn antenna

NRAO Calibration Horn Antenna 1967
Diagonal Horn Antenna; Image Source – NRAO/AUI/NSF, NRAO Calibration Horn Antenna (1967)CC BY 3.0

·       Ridged horn antenna

640px Schwarzbeck BBHA 9120 D 1
Ridged horn Antenna; Image Credit –Schwarzbeck Mess-Elektronik, Schwarzbeck BBHA 9120 DCC BY-SA 3.0

·       Dual-mode conical horn antenna

·       Septum horn antenna

·       Aperture-limited horn antenna

Horn antenna design (Pyramidal Horn Antenna)

Pyramidal horn-antenna is the most used and popular types of the horn-antenna. It is known as a standard gain horn (that is why we choose pyramidal horn for describing). The pyramidal horn’s radiation pattern is the combination of E- and H- sectoral horn-antennas. Let us discuss the design of a pyramidal horn-antenna.

Design Procedure

  • The designer/ engineer should know the gain (G0). Also the measurements of ‘a’, ‘b’, of the quadrilateral waveguide (used as feed) should be known.  
  • The designing aims to derive dimensions such as – a1, b1, ρe, ρh, Pe, Ph. The calculation should lead the designer to the optimum gain of the horn- antenna.
  • The selection of a1 and b1 should also be in a guided way so that they will help to find the optimum gain, and we can derive the design equations.
  • The efficiency of a horn- antenna including the apertures is about 50%. Now, we know that –

a1 ≈ √ (3λρ2)

b1 ≈ √ (2λρ1)

The directivity is given as – D0

D0 = Aem [ 4π / λ2]

Aem is the maximum effective area and has a relationship with the physical area (abbreviated as Ap).

Aem = εap Ap

εap is the aperture efficiency, 0 ≤ εap ≤ 1

Gain = G0

G0 = (1/2) * (4π / λ2) * (a1 b1)

Or, G0 = (2π / λ2) * √ (3λρ2) * √ (2λρ1)

Or, G0 (2π / λ2) * √ (3λρh * 2λρe) — (1)

As we assume ρ2 ≈ ρh and ρ1 ≈ ρe for long horn-antennas.

Now, to realize the physical horn- antenna, Pe and Ph must be equal.

We know that,

Pe = (b1 – b) [ (ρe / b1)2 – ¼]1/2

Ph = (a1 – a) [ (ρh / a1)2 – ¼]1/2

Now, we can rewrite the equation (1) as below.

[√ (2χ) – b/ λ]2 (2χ -1) = [{(G0 /2π√χ) * √ (3/2π)} – (a/ λ)]2 * [(G02 / 6π3χ) – 1] — (2)

Where,

ρe / λ = χ and,

ρh / λ = G02 / 8π3χ

Equation (2) is known as the horn- antenna design equation.

  1. At first, we have to calculate the value of χ, which will gratify the value of gain. An iterative approach with a trial value is considered to find out the value χ.

χ (trail) = χ1 = G0 /2π√2π

  1. Once the correct value is calculated, the value of ρe and ρh are calculated.
  2. The a1 and b1 related to the designs are calculated after that.

a1 = √ (3λρ2) ≈ √ (3λρh) = (G0 /2π) * √ (3λ/2πχ)

b1 = √ (2λρ1) ≈ √ (2λρe) = √ (2λχ)

  1. The values of pe and ph are calculated at last.

Directivity of Horn Antenna

Before we step into finding out the directivity of a horn-antenna, let us know the directivity of an antenna? An antenna’s directivity is defined as the ratio of radiation intensity of an antenna in a particular direction to the averaged radiation intensity over all the directions. Directivity is considered as a parameter for calculating the figure of merit of the antenna.

The following mathematical expression describes the directivity.

D = U / U0 = 4πU / Prad

When the direction is not given, the default direction is the direction of maximum radiation intensity.

Dmax = D0 = Umax / U0 = 4πUmax / Prad

Here, ‘D’ is the directivity, and it has no direction as it is a ratio. U is the radiation intensity. Umax is the maximum radiation intensity. U0 is the radiation intensity of the isotropic source. Prad is the total radiated power. Its unit is Watt (W).

As earlier said, the horn-antenna is of three types. All the classes have different directivity. Let us discuss all of them.

E-Plane Sectoral Horn

The following expression gives the directivity of the E-Plane horn-antenna.

DE = 4πUmax /Prad = (64aρ1 * | F(t) | 2)/πλ b1

Where, | F(t) | = [C2b1 / √ (2λρ1) + S2b1 / √ (2λρ1)]

H-Plane Sectoral Horn

The following expression gives the directivity of the H-plane sectoral horn-antenna.

DH = 4πUmax /Prad = [4πbρ2 /a1 λ]* {[ C(u) – C(v)]2 + [S(u) – S(v)]2}

Where,

u = (1/√2) * [{√ (λρ2)/a1 + a1/ √ (λρ2)}]

v = (1/√2) * [{√ (λρ2)/a1 – a1/ √ (λρ2)}]

Pyramidal Horn Antenna

The directivity of pyramidal horn- antenna depends on both the directivity of E & H plane sectoral horn. The equation is given below.

DP = 4πUmax /Prad = [8πρ1ρ2 /a1b1] * {[ C(u) – C(v)]2 + [S(u) – S(v)]2} * {[C2b1 / √ (2λρ1) + S2b1 / √ (2λρ1)]}

It can be written as –

DP = [π λ2 / 32ab] * DEDH

Horn Antenna Radiation Pattern

Radiation Pattern is the angular dependence of the strength of the radio waves from any electromagnetic source. The below image shows the radiation pattern of a pyramidal horn-antenna.

Pyramidal Horn Antenna Radiation Patterns 1

Image depicting Horn antenna radiation pattern

Horn Antenna Gain

An antenna’s gain would refer to as the ratio of the intensity in a particular direction to the radiation intensity if the antenna were radiated isotopically. It is an essential parameter for measuring an antenna’s performance and has a close relationship with the antenna’s directivity. The gain of a horn- antenna lies around 25 dBi and the range is typically 10 – 20 dBi.

Horn antenna beamwidth

Antenna bandwidth is the angular distance between two matching points on the reverse side of the outline supreme. The horn-antenna beamwidth gets decreased if the frequency of the process gets increased.

The bandwidth of a practical horn-antenna stays in a range of 10:1 to 20:1.

Few mathematical problems related to Horn Antenna

1. Find the directivity of the E-plane sectoral horn-antenna. The details for the antenna are given below. a = 0.5λ, b = 0.25λ, b1 = 6λ, ρ1 = 6λ

Solution:

b1 / √ (2λρ1) = 6λ / √ (2λ*6λ) = 6 / √12 = 1.73

Frensel 1 1

A part of Fresnel Integral Chart; Image Credit – A. VAN WIJNGAARDEN and W. L. SCHEEN

Now, [C (1.73)]2 = (0.32)2 = 0.1024 [from the chart of Fresnel integrals]

And, [S (1.73)]2 = (0.54)2 = 0.2916 [from the chart of Fresnel integrals]

We know that, DE = 4πUmax /Prad = (64aρ1 * | F(t) | 2)/πλb1

Where, | F(t) | = [C2b1 / √ (2λρ1) + S2b1 / √ (2λρ1)]

DE = [{64 (0.5) * 6 * (0.1024 + 0.2916)} / 6π]

Or, DE = 4.01 dB.

So, the directivity of the given E-Plane Sectoral Horn-Antenna is 4.01 dB.

2. Find the directivity of the H-plane sectoral horn-antenna. The details of the antenna are given below. a = 0.5λ, b = 0.25λ, a1 = 6λ, ρ2 = 6λ

Solution:

We know that,

u = (1/√2) * [{√ (λρ2)/a1 + a1/ √ (λρ2)}]

v = (1/√2) * [{√ (λρ2)/a1 – a1/ √ (λρ2)}]

Now, u = (1/√2) * [{√ (6)/6 + 6/ √ (6)}] = 2.02

And, v = (1/√2) * [{√ (6)/6 – 6/ √ (6)}] = – 1.44

Using Fresnel integrals,

C (u) = C (2.02) = 0.48825

C (v) = C (-1.44) = -C (1.44) = – 0.54310

S (u) = S (2.02) = 0.3434

S (v) = S (-1.44) = -S (1.44) = – 0.71353

We know that directivity of H-plane sectoral horn- antenna is 

DH = 4πUmax /Prad = [4πbρ2 /a1 λ]* {[C(u) – C(v)]2 + [S(u) – S(v)]2}

Or, DH = [4π (0.25)6/6] * [ (0.488 + 0.543)2 + (0.343 + 0.713)2]

Or, DH = (3.141) * (1.0629 + 1.1151)

Or, DH = 6.84 dB

So, the directivity of the given H-plane Sectoral Horn-Antenna is 6.84 dB.

3. Designing details of a pyramidal horn-antenna is given below. ρ2 = 6λ = ρ1 = 6λ; a = 0.5λ, b = 0.25λ; a1 = 6λ = b1 = 6λ; Check if a practical horn-antenna can be designed with those details. Also, find out the directivity of the pyramidal horn- antenna.

Solution:

            Now, ρe = λ √ ([62+ (6 / 2)2] = 6.708λ

            And, ρh = λ √ ([62+ (6 / 2)2] = 6.708λ

We know that,

Pe = (b1 – b) [ (ρe / b1)2 – ¼]1/2

Ph = (a1 – a) [ (ρh / a1)2 – ¼]1/2

Now, Pe = (6λ– 0.25λ) [ (6.708 / 6)2 – ¼]1/2 = 5.74λ

And, Ph = (6λ– 0.5λ) [ (6.708 / 6)2 – ¼]1/2 = 5.12λ

As we can see, Pe is not equal to Ph, so the design is not possible to implement.

            We know that the directivity of a pyramidal horn-antenna is 

DP = [π λ2 / 32ab] * DEDH

            Now, DP = [π / 32 * (0.5) * (0.25)] * 6.84 * 4.01]

            [The value of DEDH is has been calculated previously]

            Or, DP = 21.54

            Converting it to the dB value, DP = 10log21.54 = 13.33 dB

So, the directivity of the given Pyramidal Horn-antenna is 13.33 dB.

Nanofluid: 17 Important Explanations

nanofluid 291x300 1

Following contents are explained in this articles:

  • Nanofluid definition | what is nanofluid?
  • What is base fluid?
  • How do you make a Nanofluid?
  • What is hybrid nanofluid?
  • Uses of nanofluid | applications of nanofluid
  • Types of nanofluid & Its Poperties

Nanofluid definition | What is nanofluid?

Nanofluid is fluid that consists of a base fluid with nanosized particles (1–100nm) suspended in it. Nano particles used in this type of studies are made of a metal or metal oxide, increase conduction and convection, allowing for more heat transfer. In the past few years, high-speed advancement in nanotechnology has made emerging of new generation coolants called nanofluid.

Let’s take example, check figure below. The CuO (metal oxide) nanoparticles are added to make nanofluid with a volume fraction of 0.25% CuO. The nanoparticle is dispersed in distilled water (base fluid). The surfactant sodium dodecyl sulfate (SDS) is added to the nanofluid for the stability of nanoparticles.

Figure 1. Nanofluid
CuO Nanofluid

What is base fluid?

The nanoparticles are suspended in some ordinary liquid coolant like distilled water, ethylene glycol, oil, refrigerants, etc. This widely used ordinary coolant is known as base fluid.

You might have noticed while mechanic changing or pouring coolant in your car radiator. Do you remember its color? Yes, it’s green. That green colored fluid (coolant) is ethylene glycol.

Let’s know about base fluid oil. You might have noticed mechanic changing oil from your car or bike. It is lubrication and transmission system oil. This type of oil can be base fluid for nanofluid preparation.

How do you make a Nanofluid?

                The preparation of nanofluid can be possible by following two widely used methods. It is prepared by dispersing nanoparticles in base fluid with a magnetic stirrer and sonicator, as shown in figure “Preparation of nanofluid : Sonicator”.

                There are two types of stirrer used to disperse particles into basefluid, one is the magnetic and another is mechanical. The another lab instrument called ultrasonic sonicator is also required for proper dispersion.

preparation 1 1
Preparation of nanofluid : magnetic stirrer

preparation 2
Preparation of nanofluid : Sonicator

Two-step method

The two-step procedure is the most widely used method for preparing nanofluid. The chemical and physical peocesses are used to produce dry powder of nanoparticles.

The powder of particles is added into the base fluid. The second step could be intensive magnetic force agitation or ultrasonic agitation. The two-step procedure is the economic procedure to produce nanofluid on  bulk because the nano fluid requirements are raising with new applications.

Use of surfactant in nanofluid

The nanoparticles have large surface area and surface activity which lead to aggregate. The use of surfactant is convenient method to get good stability. However, the surfactants’ functionality under high temperatures is also a big issue, especially for high-temperature applications.

One-step method

Eastman suggested a one-step method of vapor condensation. It is used prepare Cu/ethylene glycol (EG) nanofluid to limit the agglomeration of nanoparticles.

The use of one-step preparation method avoid spreading the particles in the fluid. There are some function not needed in this method. This method eliminates drying of particles, storage of material, and spreading. Agglomeration is limited in one -step method. it also increases stability of nanofluid.

Vacuum method – SANSS

 (full form Submerged -arc -nanoparticle -synthesis- system)

It is one of the preparation method of nanofluid with good efficiency. Different dielectric fluid are used in this method

The shape of nanoparticles are like different different type. The procedure avoids the undesired particle aggregation reasonably well. There are some disadvantages of this method. There is some reactant remain present in nanofluid.

What is a hybrid nanofluid?

A hybrid material is a combination of physical and chemical properties of two or more materials. The two or more nanoparticles are dispersed in a base fluid to achieve desired properties for individual applications. The making of nanofluid with two or more similar or different nanoparticles is popular as hybrid nanofluid. The work on hybrid nanofluid is not extensively done.

There are many experimental studies on hybrid nanofluid is still left to be done. The generally used hybrid nanofluids are Al2O3/Cu, Al2O3/CNT, Cu/TiO2, CNT/Fe3O4, etc.

The hybrid nanofluid is a new research area for thermal engineering researcher to obtain enhanced cooling system.

Usage of nanofluid

                Nanofluid can be utilized for various different applications. These uses not affecting energy transfer thoroughly, they may be reduce the basic need for conventional fuel, electrical energy, or gas. Let’s read some important application of nanofluids

Electronic devices cooling

               The research going on the electronics suggests that the use of nanofluid can perform superior heat transfer. The vapour chamber is utilizing nanofluid in it for better heat transfer.

Jacket-water fluid in electricity generator

               The management of machinery space is main problem in all automobile vehicle. The size of component (cooling) can be reduced only if we improve heat transfer performance of parts. The nanofluid is the one of the option to improve performance of part and develop compactness.

Solar energy – thermal energy system

                To absorb solar radiation, the working fluid is passes through solar thermal energy system. The energy absorbed by fluid is sent to heat exchanger for other purposes.The solar energy absorbed by working fluid is generally transferred to the heat exchanger for other applications.

Cooling oil in Transformer

                The transformer is power transmission electrical equipment. The generated heat in transformer is absorbed by oil. If we add nanoparticle in cooling oil. The performance of transformer can be improved.

Other usage of nanofluid in the field of heat transfer enhancement:

Refrigeration process

                The refrigeration process is working on different thermodynamic cycles.  The working fluid in this process is refrigerant. The thermal properties of some refrigerant can be improved by use of nanoparticle.

Cooling system of nuclear energy

                The huge amount of heat is produced in the nuclear fission. It is required to arrange proper cooling to system. The nano fluid is advance fluid which can be utilized in nuclear cooling system.

Types of nanofluid

The types of nanofluid are dependent on the use of different types of nanoparticles and base fluids. There are three types of nanoparticles, like pure metal, metal oxide, and carbide-based nanoparticles. These particles are dispersed in various choices of base fluids like water, water/ethylene glycol, oil, ethylene glycol, etc.

Pure Metal Metal oxides Carbide
Al Al2O3 Diamond
Cu CuO Graphite
Fe Fe2O3, Fe3O4 Single wall nanotube
Ag Ag2O Multiwall nanotubes
Zn ZnO  
Ti TiO2  

Properties of nanofluid

Thermal conductivity is one of the vital property related to heat transfer for nanofluid. It is high thermal conductivity compared to standard cooling liquid, it is an essential characteristic for many applications. Use of copper nanoparticles with ethylene glycol results in an increase in thermal conductivity by 40% compared to the base fluid.

All processes indicates that thermal conductivity basic for proper cooling system in any devices. In the cooling system, a large surface area and high thermal conductivity are attributed to this heat transfer improvement.

The ratio of surface area and volume is main criteria for thermal conductivity improvement. This ration can be increased by using small size nanoparticles. The thermal conductivity is raised by using higher concentration of the particles.

The properties like density, viscosity, specific heat, thermal conductivity are well known for base fluid. The properties of nanofluid can be calculated theoretically by correlations suggested by various researchers. These properties also can be measured with multiple instruments experimentally in the lab.

The density of nanofluid can be calculated using correlation as  

\rho_{n}f=(1-\Phi)\rho_{b}f+\Phi{\rho_{p}}

Where ρpand ρbfare the nanoparticles’ densities and base fluid, respectively, and фis the volume concentration (% w/w) of nanoparticles dispersed in the base fluid. As per the idea of the strong fluid combination, the specific heat of nanofluid is given by the accompanying:

{ C }p_{ nf }=\quad \frac { (1-\phi ){ \rho }_{ bf }\quad { Cp }_{ bf }+\phi \quad { \rho }_{ p }{ Cp }_{ p } }{ { \rho }_{ nf } }

Where cppand cpbf, are the specific heat of the nanoparticles and base fluid, respectively. The viscosity of nanofluid can be obtained from the following equation:

{\mu}_{nf}={\mu}_{bf}(1+a\phi)

Credit Einstein 1906

 a is constant in viscosity equation and its  value is 14.4150 to  calculate viscosity. This formula is basically given for Brownian motion of particle in fluid. One well-known formula for computing the thermal conductivity of nanofluid is the Kang model which is expressed in the following form :

K_{ nf }=\quad { K }_{ bf }\frac { { K }_{ p }+(n-1){ K }_{ bf }-\phi \quad (n-1)\quad ({ K }_{ bf }-{ K }_{ p }) }{ { K }_{ p }+(n-1){ K }_{ bf }+\phi\quad ({ K }_{ bf }-{ K }_{ p }) }

Credit Hamilton and Crosser (1962)

Question and Answers

What is nanofluid?

It is an advance fluid. It is prepared by dispersing nanoparticles in the base fluid.

What is base fluid?

 The base fluid is conventional coolant liquid. It is used to prepare nanofluid.

Give the examples of some commonly used nanoparticles to prepare nanofluid.

The commonly used nanoparticles are Copper (Cu), Aluminium (Al), Iron (Fe), Aluminium Oxide (Al2O3), Copper Oxide (CuO), Titanium Oxide (TiO2 ) etc.

What are widely used preparation methods of nanofluid?

There are two methods widely used mentioned as below:

  1. Two-step method
  2. One-step method

What is the stability of nanofluid?

The stability can be stated as how long the particle keep dispersed in the base fluid. Technically, The higher stable nanofluid is one who has less sedimentation.

What is the use of surfactant in preparation of nanofluid?

The surfactant is used in nanofluid to increase its stability. The commonly used surfactant is sodium dodecyl sulfate (SDS).

Why hybrid nanofluid became a new research topic?

The individual application needs the desired properties of the material. To get likely properties in nanofluid, more than one nanoparticles are added in the base fluid.

Why the use of nanofluid results enhanced heat transfer?

The nanofluid is an advanced fluid with a higher thermal conductivity as the nanosized particles provide more surface area to conduct heat transfer.

How can nanofluid reduce the size of the heat exchanger?

The convention coolant used in heat exchanger shows less heat transfer as compared to nanofluid. The use of nanofluid requires proportionally less sized heat exchanger as compared to the conventional coolant.

Conclusion

                This article is about basic introduction of nanofluid, preparation of nanofluid, application of nanofluid and properties of nanofluid. Recently, it is advance coolant in heat transfer applications. The scope of nanofluid is vast in present nanotechnology world. The nanofluid and its applications can be a good topic for students and researcher for project work.

For more details regarding it, please refer click here

More topic related to Nanofluid and heat transfer, please click here

Transmission Line: 5 Facts You Should Know

TINE

Cover Image Credit – Sajad-HasanAhmadiTV antenna connectorsCC BY-SA 4.0

Points of Discussion: Transmission Line

  • Introduction
  • Purpose of transmission line
  • Analysis of transmission line
  • Types of transmission line
  • Applications of transmission lines

Introduction to Transmission Line

A transmission line is a specially designed cable for transmission of power. It conducts only electromagnetic waves to the load at low frequencies in a guided way.

            Transmission line operates at microwave frequency domain and radio frequency domain where power is assumed as an electromagnetic wave. That is why if any cable can guide an electromagnet signal, then it will be called a Transmission line.

            The transmission line is the result of researches of James Maxwell, Lord Kelvin, and Oliver Heaviside. The fault and drawbacks of the ‘Atlantic telegraph cable’ and invention of telegrapher’s equation made the way out for the line.

Purpose of transmission line

Regular cables which transfer electrical energy are designed to conduct power at lower frequency AC. They cannot carry power in FR range or above 30 kilo hertz as the energy gets disconnected at joints and connectors, and some time does not reach the destination. This lines resolve these problems. They are constructed specially to minimize the reflections and loss of power and also uses the impedance matching to carry power.

            This lines are constructed with a uniform cross-sectional area. That is why they provide uniform impedance which is in terms known as characteristic impedance.

Transmission Line

Use of Transmission Line in antenna

            The wavelength of the electromagnetic waves gets shorter as the frequency gets higher of the electromagnetic waves.  Transmission lines are crucial because when the wavelength is short enough, the length of the wire contributes to the past of the wavelength.

What is a Yagi Uda Antenna? Click here for details!

Analysis of Transmission line

            We assume a four-terminal model of the transmission lines to analyze the construction and working of lines. It is equivalent to a typical two-port circuit. 

            We assume that the circuit is linear, which means that the complex voltage at any port is relational to the complex current for the reflectionless condition. Also, we assume that two of its ports are transposable.

Characteristics impedance of transmission line

Characteristic impedance or (Z0) is an essential parameter of the line. It can be defined as the ratio of the magnitude of the voltage to the magnitude of the current of a wave, travelling along a reflection less line.

Characteristics impedance controls the behaviors of the line only if the line is uniform in length. Generally, for co-axial cables, characteristic impedance has a value of fifty to seventy ohms, and for warped pair of wires, the value is 100 ohms. For untwisted pair, the value is 300 ohms.

Transmission line reflection coefficient

The line’s reflection coefficient is given by the ratio of the complex magnitude of the reflected signal to the incoming signal. It is represented by the Greek alphabet – Г and expressed as –

Transmission line reflection coefficient

where V+ is the complex voltage of the incoming voltage and  V- is the complex voltage of the reflected wave.

It has a relation with the load impedance and characteristic impedance. The expression is given below.

Transmission line

Here ZL is the load impedance, and Z0 is the characteristic impedance.

The standing wave ratio also has a relation with this line reflection coefficient. The connection is given as –

Transmission line

The relation between Standing Wave Ratio and transmission line reflection coefficient.

Matched condition of transmission line:

The aim of a transmission line is to deliver the maximum power from the source to destination load and to minimize the reflection and loss of the power. The ‘matched’ condition can fulfil this desired. If the destination’s load impedance is made same or equal to the value of the characteristic impedance of the line, then the line achieves ‘matched’ condition.

            Instead of the ‘matched’ condition, the transmission suffers some loss. Like, ohmic loss. There is also another substantial loss that occurs when this line works in high frequency ranges. The loss is known as dielectric loss. Here, the inside elements of this lines, grips the EM energy and produces heat.

            The aggregate loss of this line is measured by the unit dB/m. The losses are dependent on the frequency of the signal, as mentioned earlier. The constructor companies of this usually provide a chart of loss. It shows the loss of power at different frequencies. If any line suffers a loss of three decibel/meter, then the power received at the load will be half of the power supplied.

What is horn antenna? get an overview here!

Types of transmission lines

 These come with certain types depending upon its physical structure and according to the needs. Some of the essential and widely used types of transmission lines are listed below. Please go through it and discover them.

Co-axial cables:

It is one of the widely used forms of lines. It restricts the whole EM wave inside the cable. Thus, co-axial cables can be bent, strapped as well as twisted to an extent without affecting the operation.

Co axial cable

Cross-section of a Co-axial Cables, Image Credit: Tkgd2007Coaxial cable cutawayCC BY 3.0

EM waves promulgate in TEM or transverse electric and magnetic mode For the RF range applications. Here, both the electric and magnetic fields are perpendicular with the promulgate directions. The electric field becomes radiated, and the magnetic field becomes circumferential.

If the wavelength of the wave is shorter than the circumference of the co-axial cable, then the TEM gets divided into two. The modes are then known as TE or transverse electric and TM or transverse magnetic.

Co-axial cables have broad applications for televisions. It was primarily used for telephones in the middle of twenty century.

Microstrip transmission lines:

A microstrip network is basically a tiny conductive plane, placed parallelly to the ground surface. It can be designed by putting a thin and flat metallic plane on the side of a PCB. The opposite surface must be the ground plane. The characteristic impedance of the microstrip type line depends on that conductive strip. The height, width, dielectric coefficient of the conductive strip provides the characteristic impedance. A point to be remembered that the microstrip type line is an open structure while the co-axial cable is a closed one.

640px Electric and Magnetic Fields for Microstrip.svg

Electric & Magnetic field of Microstrip Transmission Line,

Image Credit: Dassault

Twisted pair transmission lines:

In this type of line where pairs of wire are assembled together to form a single chain or a cable is known as tangled pair transmission lines. These types of lines are used in global telephonic communications. Also, it has used in data circulation inside buildings. This type is not economical due to its properties.

640px Twisted pair.svg

Image of a Twisted Pair types. Image Credit – Spinningspark at en.wikipediaTwisted pairCC BY-SA 3.0

Star quad:

Star quad is another wire-combinational formation. It uses four cables, and all the conductors of the four cables are twisted and assembled along the axis of the cable. In this formation, each and every pairs uses a far pair to get connected.

The combinational form of twisted, balancing and quadrupole pattern of transmission lines has several benefits as it reduces noise, particularly for short signal level usage like – cables of the microphone.

Transmission line

Descriptive image of a star quad cable, Image Source – Spinningspark at en.wikipediaDM quadCC BY-SA 3.0

This type of line has applications in four-wire telephony, two-wire applications.

It also induces high capacitance which further causes distortion and losses.

Applications of transmission lines | Uses of transmission lines

Transmission lines have several benefits over regular electrical cables in specific domains. That is why it has several applications. Let us discuss some of them.

  • Electromagnetic powers are supplied in high frequency domains with minimum loss. Tv and radio cables for connecting the aerials is one of the most famous examples.
  • These are also used for the generation of pulses by charging and discharging this lines. A significant example of this type of line is – Blumlein Transmission Line. Radars have also multiple application of this kind.
  • These are also applied in stub filters. Stub filters are typically wired in a parallel connection and transfer power from the source to destinations.

Check out more on Electronics! Click Here!

Pulse Code Modulation (PCM): 7 Complete Quick Facts

PCM Sampling 300x225 1

The subject of Discussion: Pulse Code Modulation (PCM)

  • What is Pulse Code Modulation?
  • Important features of PCM
  • Sampling Method in Pulse Code Modulation (PCM)
  • Encoding in Pulse Code Modulation (PCM)
  • What is Quantization?
  • Advantages of PCM
  • Disadvantages of PCM
  • Important applications of Pulse Code Modulation (PCM)

What is Pulse Code Modulation?

Definition of PCM:

Pulse code modulation or PCM is a distinct type of A-to-D conversion method in which the data or info enclosed in the samples of an analog signal is obtainable by a digital procedures.”

In this method, each of the digital signals has n number of binary digits, there are M= 2n unique number of code is possible, and all these codes have a specific amplitude level. However, for each sample significance from the analog signal could be any one of an unlimited levels.

The digitally encrypted word characterized by the amplitude closest to the actual sampled value is used. This is named as quantizing and process entitled as quantization. As an alternative of using the similar sample value of the analog form w(kTs), the nearby allowable value substitutes the sample, where there are M allowed values, each corresponding to one of the code words. Other widespread categories of A-to-D conversions, i.e, Delta-modulation (DM) and the differential pulse code modulation (DPCM), are discussed later.

Important features of Pulse Code Modulation:

Pulse coded modulation has various features. Some of the important features of Pulse Code Modulation are the following:

  • PCM technique is comparatively cheap digital circuitry and could have used extensively for various applications.
  • Pulse Code Modulation signal is resulting from all categories of analog signal (vedio, audiovisual, etc.) combination with data signal (i.e., available from the digital computers or laptop) and communicated over a standard fast-speed digital telecommunication scheme. This multiplexing technique is called TDM and is talk over in a separate section.
  • In a distanced digital telecommunication schemes requiring a repeaters, a clean PCM signal restored at the each repeater’s o/p, where the i/p be made up of PCM pulse mixed with noise. Nevertheless, the noise in the i/p signal might create o/p bit-errors in the PCM technique.
  • The signal-noise ratio of a digital system could have improved in comparison to the analog system. The error probability in the system output could be minimized even further by using proper coding based encryption technique. This compensate the main disadvantage of PCM; a much broader bandwidth range than the analogous analog techniques is requirement.

Sampling, Quantizing and Encoding in PCM:

The Pulse Code Modulation signal is generated from the quantized Pulse Amplitude Modulated signal. Quantized values are encoded here.

Generally, a system designer is designated to state the same code word or encryption represented by a specific quantized level for a Gray code. In this resulting Pulse Code Modulation signal, this word or byte for every quantized sample is strobed out the encoder by the next immediate pulse. The Gray code is utilized because, in this, only a one-bit will alter for each step of quantization. Typically, the ‘errors’ in the received PCM signal will cause minimal errors in the received analog signal, provided that the sign bit is not in error.

PCM methods exemplify the quantized analog sample value by the binary codes. As a general rule, it is probable to define the quantized analog samples by digital words using a base other than ‘2’ or, evenly, to transform the binary to other multi-level signal.

PCM Sampling
This image shows the process of sampling and quantization. Image Credit :anonymous, PcmCC BY-SA 3.0

Operations in the Transmitter:

Sampling

The message signals pass under a process of sampling where they are sampled by the pulse signals. To reform the signal back to its original form, there is a specific condition for sampling rate. The rate must be the multiple of 2 or more of the greatest frequency component present in the signal.

Nyquist’s theorem is one of the important rule in the process of sampling. It deals with the sampling rate and necessary conditions for reconstruction of a signal after being sampled. The theorem is important not only for the Pulse Coded Modulations, but also for each and every modulation techniques and for every aspects of signal theories and signal applications. Mathematically, it says:

Fs >= 2 * Fmax

Here, Fs is the frequency of sampling and Fmax is the value of the greatest frequency component present in the signal.

Antialiasing filters plays a major role here. They omits specific frequency bands which are generally higher than the W.

Three different sampling methods
Three different sampling methods
Image credit : Dr.J.L Mazher Iqbal Slideplayer Presentation

Encoding

Encoding refers to the process of conversion by which datas are symbolised through some specific symbols, or characters. This process brings more security to the communication system. That is why the process is important. For long transmission there is always possibility of unwanted interferences. Encoding saves us from those attacks.

In Pulse Coded modulation technique of transmission, the analog datas are converted to the digital signal. This part of operation is one of the important stage. It can be also stated as the ‘Stage of Digitization’.

The constant communication signal gets converted to distinct values. This distinct procedures in a code is called a code element or symbol. A code element or symbol is given by the discrete events in a code. As we know, the binary codes are given by Zeros and Ones.

Quantization

 “The Quantizing is a procedure of minimizing the extra unnecessary bits and limiting the data.”

State the advantages and disadvantages of PCM:

Advantages  of PCM

  • It transmits signals uniformly.
  • PCM has an efficient SNR.
  • PCM always offers efficient regeneration.

Disadvantages of PCM

  • Attenuation occurs due to noise and cross-talks.
  • PCM needs a larger bandwidth for transmission.
  • Other errors are also observed during transmission.

For more electronics related article click here

Pulse Amplitude Modulation (PAM): 5 Important Explanations

flat top 300x287 1

Subject of Discussion: Pulse Amplitude Modulation (PAM)

  • What is pulse amplitude modulation?
  • Flat top and natural PAM
  • What is PWM and PPM
  • Advantages and disadvantages of PAM
  • Comparison of PAM vs PWM vs PPM

What is Pulse Amplitude Modulation?

Definition of Pulse Amplitude Modulation:

“The modulation technique which is utilized to state the transfiguration of the analog signal to a pulse-type signals in that the amplitude of the pulse signifies the analog info”.

The modulator performs the primary steps while the conversion of analog signal to a Pulse Code Modulated Signal. In a number of application the Pulse Amplitude Modulation signal is used directly and complex conversion such as PCM is not at all required.

Types of Pulse Analog Modulation

The Pulse Analog Modulation can be classified into three categories. They are –

  1. Pulse Amplitude Modulation (PAM)
  2. Pulse width Modulation (PWM)
  3. Pulse Position Modulation

The relation between the pulse and constant amplitude of the message signal is proportional. As explained here, PAM is to a certain extent analogous to natural sampling technique, in which the message signal is multiplied by a periodic square pulses. In regular sampling process, however, the modulated square pulse is acceptable to vary with the message signal, however in pulse-amplitude modulation it is retained as flat signal.

 

Types of Pulse Amplitude Modulation

Pam can be categorized into two categories. They are – Flattop Pulse Amplitude Modulation and Natural Pulse amplitude modulation.

Flat Top Pulse Amplitude modulation:

The pulses’ amplitudes are dependent on the amplitude of the message signal.

Flat Top Pulse Amplitude modulation
Flat Top Pulse Amplitude modulation

Natural PAM:

Natural Pulse Amplitude modulation
Natural Pulse Amplitude modulation

Write down some of the Applications of PAM?

Applications of PAM

There are several applications of Pulse Amplitude modulation such as

  • PAM is used in Ethernet Communication.
  • PAM is used in many micro-controllers to generate some control signals.
  • In Photo-biology system, PAM is also used.

What are the advantages of PAM?

Advantages of Pulse Amplitude modulation

  • Pam is a better straightforward, less complex process for the modulations as well as demodulations.
  • The design of transmitters and receivers of PAM is quite a straightforward job and less complex than other design. 
  • Pulse Amplitude Modulation be able to produce other pulse modulation signals and transport the message signal at that time.

What are the disadvantages of PAM?

Disadvantages of Pulse Amplitude modulation

  • For PAM, bandwidth should be larger for transmission.
  • PAM has a great noise problem.
  • The PAM signal will changes, so that the power requisite for transmission may increase.

What is Pulse Width Modulation?

Definition of Pulse Width Modulation (PWM):

  •  “This is an analog modulating technique in which the duration, width, and time of the pulse carrier will be changed in proportion to the amplitude of the message signals.”
  • The pulses’ widths change in this technique. Though pulse’s magnitude remains the same.
  • In PWM, amplitude limiters are utilized as to create the amplitude of the signal as constant.

This PWM is also recognized as a Pulse Duration Modulation (PDM) and the Pulse Time Modulation (PTM) technique.

PWM
Pulse Width Modulation
An example of PWM in an idealized inductor driven by a voltage source modulated as a series of pulses, resulting in a sine-like current in the inductor.
Image source – ZureksPWM, 3-levelCC BY-SA 3.0
delta PWM
Principle of the delta PWM. Output signal (blue), limits (green).

Image Credit: Delta_PWM.png: Cyril BUTTAY derivative work: Krishnavedala (talk), Delta PWMCC BY-SA 3.0
Sigma Delta PWM

Image Credit :Sigma_delta.png: Cyril BUTTAY derivative work: Krishnavedala (talk), Sigma-delta PWMCC BY-SA 3.0

What is Pulse Position Modulation?

Definition of Pulse Position Modulation (PPM):

In the pulse-amplitude modulation or pulse-width modulation or pulse-length modulation technique, the pulse amplitude is the variable parameter, so it changes. The pulse’s period is one of the important parameter. The modulating signal is changes with the time of incidence of the leading or trailing edges, or both edges of the pulse.

Comparative analysis of PAM, PWM and PPM:

            PAM            PWM             PPM
In PAM amplitude keeps varying.In case of pulse amplitude modulation, the BW is dependent on the width of the following pulse.In PPM, the BW of the pulse is dependent on the rising-time of the pulse.
In PAM, the bandwidth depends on the width of the following pulse.In Pulse Width Modulation, Bandwidth is depended on the rising time of the pulseIn PPM, Bandwidth is depended on the rise time of the pulse
In Pulse amplitude Modulation (PAM) , System or circuit design is complex.In Pulse width modulation (PWM), System or circuit design is less complex.In Pulse position modulation (PPM), System or circuit design is less complex.
  High noise interference  Low noise interference  Low noise interference

For more electronics related article click here

Read more about Amplitude Modulation and Demodulation.

Strength of Materials: 27 Complete Quick Facts

e1

There are two types of body: rigid body and deformable-body. Distance between any two points remains constant with force applied on a body is known as a rigid body and the body in which this distance change is known as a deformable body. Strength of material is the study of deformable bodies.  In this, we study the different properties of materials by applying force on it. Study of the strength of materials helps to select material for different applications according to their properties. Strength of Material is also referred as Mechanics of Material. Strength of Material includes stress, strain, stress-strain curve etc.

Engineering Stress

  • Instantaneous load or force applied per unit original area of cross-section (Before any deformation) is known as engineering stress.
  •  It is denoted by σ (sigma). SI unit of engineering stress is N/m2 or Pascal (Pa).

Engineering Stress= (Force Applied)/ (Original Area)

Strength of Material: Engineering Stress
Strength of Materials: Engineering Stress
Strength of Materials : Engineering Stress

Click Here! for more details

Classification of Stress

Generally following engineering stresses are classified in strength of materials studies.

Strength of Material : Classification of Engineering Stress
Strength of Materials : Classification of Stresses

Normal Stress

  • When the applied force is perpendicular to the given cross-section of the specimen (axial load), then the corresponding stress produced in the material is known as normal stress.
  •  Many times force applied on the surface is not uniform; in that case, we take an average of the applied force.

Normal Stress= (Perpendicular component of Applied Force)/ Area

Strength of Material: Normal Stress

Tensile Stress

When the applied force is away from the material, then the Stress produced is known as tensile stress.

Strength of Material: Tensile Stress
Strength of Materials : Tensile Stress

Compressive Stress

When the applied force is in towards the object, then the Stress produced is known as compression stress.

Strength of material: Compressive Stress
Strength of Materials: Compressive Stress

Bending Stress

  • When force is applied on the beam-shaped material, the material’s top surface undergoes a compressive type of stress, and the bottom surface undergoes tension-type of Stress and middle of the beam remains neutral. Such stress is known as bending Stress.
  •  It is also known as flexural Stress.
Strength of Material: Bending Stress
Strength of Materials: Bending Stress

Shear Stress

When the applied force is parallel to the area on which it is applied, the Stress is known as shear stress.

Strength of Material: Shear Stress
Strength of Materials : Shear Stress

Shear Stress Formula

Shear Stress= (Force imposed parallel to the upper and lower faces) / Area.

Strength of Material: Shear Stress

Tensile Stress vs Shear Stress

Tensile StressShear Stress
The applied force is perpendicular to the surface.The applied force is parallel to the surface.
It is denoted by σ.It is denoted by τ.

Combined Stress Equation

While studying strength of materials in real-life examples, we can have cases in which more than one type of Stress is acting on the material, in that case, we need to have an equation which can combine different type of stresses

Following is the equation which combines shear and tensile stresses.

Strength of Material: Combined Stress Equation

Where,

fx= tensile or compressive stress in the x-direction

fy= tensile or compressive stress in the y-direction

fs= shear stresses acting on the faces in x and y-direction

f1= maximum principle Stress

f2= minimum tensile Stress

q= maximum shear stress

Stress Concentration Factor

  • In the studies of Strength of Materials, many times the material on which we are applying Stress is not uniform. It may have some irregularities in its geometry or within the structure formed due to nicks, scratches holes, fillets, grooves, etc., which causes the concentration of stress to be very high at some point on the material known as stress concentration or stress riser/raiser.
  • The degree of this concentration is expressed as the ratio of maximum Stress to reference Stress, where reference stress is total Stress within an element under the same loading conditions, without any concentration or discontinuity.

Stress Concentration Factor Formula:

Stress Concentration= maximum Stress / Reference Stress

Strength of Material: Stress Concentration Factor

Click Here! for more details

Factor of Safety

  • While studying strength of Materials, there are always some uncertainties in the measured values of stresses; therefore, the stress that we are going to consider for our use known as working stress (σw) is always less than the experimental value of stress. In most of the applications, we consider yield strength (σy).
  • Working Stress is determined by reducing the yield strength by a factor; that factor is known as the factor of safety. So, the factor of safety is a ratio of yield strength to working stress. Its symbol is N. It is a unitless quantity.

            Factor of Safety= Yield Strength/ Working Stress

Strength of Material: Factor of Safety

Engineering Strain

  • Change in length at some instant of the material per unit original length (Before any application of force) is known as engineering strain.
  •  It is denoted by ε (Epsilon) or γ (Gamma). It’s a unitless quantity.

              Engineering Strain= (Change in length)/ (Original Length)

Strength of Material: Engineering Strain Formula
Strength of Material: Engineering Strain
Strength of Materials : Engineering Strain

Poisson’s Ratio

  • When tensile stress is applied to the material, there is elongation along the applied load axis and shortening along with perpendicular directions to the applied Stress. Thus, the strain produced in the applied stress direction is known as axial strain and the strain produced in the perpendicular direction the applied Stress is known as lateral strain or transverse strain.
  • The ratioof the lateral strain and axial strain is known as Poisson’s Ratio. It is denoted by ʋ (nu). It is a very important constant for a given material.

            Poisson’s Ratio= – (Lateral Strain/ Axial Strain)

Let the applied load is in z-direction and strain produced in that direction is εx  and  material is isotropic and homogeneous ( ) then Poisson’s ratio is

Strength of Material: Poisson's Ratio Formula
Strength of Material: Poisson's Ratio
Strength of Materials : Poisson’s Ratio

To learn in detail on Poisson’s Ratio Visit here

Stress-Strain Curve

  • Plotting of stress to strain gives a considerable number of properties of the material in strength of materials study.
  • The stress-strain curve is stress versus strain curve in which strain is on independent axis i.e., x-axis and stress is on dependent i.e. y-axis. It is an important characteristic of the material.
  • On the load application, two types of deformation occur in the material depending upon the strain value, first is elastic deformation and second is plastic deformation.
Strength of Material: Stress-Strain Curve
Strength of Materials: Stress-Strain Curve

True Stress-Strain Curve

It is a stress-strain curve in which true Stress is plotted against true strain. Both Stress and strain are based on instantaneous measurement. Hence, the instantaneous cross-section area is considered instead of original cross-section, and instantaneous length is considered instead of the original length.

Elastic Deformation

  • Elastic deformation is the deformation in which material regains its original shape on the removal of the force.
  • This region has a proportional limit, elastic limit, upper yield point and lower yield point.

Modulus of Elasticity | Hooke’s Law

  • When this type of deformation occurs, the strain in the metal piece is nearly proportional to the stress; therefore, this deformation occurs as a straight line in Stress versus strain plot except for some materials like grey cast iron, concrete and many polymers.
  • Stress is proportional to the strain through this relationship.
Strength of Material: Hooke's Law
  • This is known as Hooke’s Law, where Y the proportionality constant is known as Young’s Modulus or Modulus of Elasticity. It is also denoted by E. It is the slope of the stress-strain curve in the elastic limit. It is one of the most important law in the studies of strength of material.

Modulus of Elasticity Formula

Modulus of Elasticity Formula

Its value is slightly higher for ceramics than metals and value is slightly lower for polymers than metals. Or most structures are required to have deformation only in the elastic limit; therefore, this region is quite important.

Plastic Deformation

  • If the applied force is removed in this region, then the material does not regain its original shape.
  • The deformation in the material is permanent.
  • In this region, Hooke’s law is not valid.
  • This region has ultimate tensile strength of materials and breaking point.
  • There are some points on the curve around which type of deformation changes. These points are very important as they tell us about the limitations and ranges of material which are ultimately useful in material’s application.

Proportional Limit

  • It is the point in the curve up to which Stress is proportional to the strain.
  • When the material is stretched beyond the proportionality limit, stress is not proportional to the strain, but still, it shows elastic behaviour.

Elastic Limit

  • It is the point in the curve up to which material shows elastic behaviour.
  • After this point, plastic deformation in the material begins.
  • Beyond the elastic limit, Stress causes the material to flow or yield.

Yield Point

It is the point where yielding of the material occurs; hence plastic deformation of material begins from this point.

What is Yield Strength?

  • Stress corresponding to the yield point is known as yield strength—its resistance to its plastic deformation.
  • Many times it is not possible to locate it precisely. The elastic-plastic transition is well-defined and very abruptly, termed as yield point phenomenon.
  • Upper Yield Point: It is the point in the graph at which maximum load or Stress required to initiate the plastic deformation of the material.
  • Lower Yield Point: It is a point at which minimum Stress or load is required to maintain the material’s plastic behavior.
  • The upper yield point is unstable, but lower yield point is stable, so we use a lower yield point while designing the components.

Ultimate Strength Definition | Ultimate Stress Definition

  • After yielding, as plastic deformation continues, it reaches a maximum limit known as ultimate Stress or ultimate strength.
  • It is also known as Ultimate Tensile Strength (UTS) or tensile strength. It is the maximum stress that can be sustained by material in tension.
  • All deformation up to this point is uniform, but at this maximum stress, small narrowing of material begins to form, this phenomenon is termed as ‘necking’.

Rupture Point | Fracture Point | Breaking Point

  • Stress necessary to continue plastic deformation starts to decrease after ultimate strength and eventually breaks the material at a point known as rupture point or fracture point.
  • The stress of the material at rupture point is known as ‘rupture strength’.

Stress-Strain curve for Brittle material

Strength of Materials : Stress Strain Curve for Brittle Materials
Strength of Materials : Stress-Strain Curve for Brittle Material

Stress-Strain Curve for Ductile Material

Stress-Strain Curve for Ductile Material
Strength of Materials : Stress-Strain Curve Ductile Material

 Ref. – Stress-Strain

Important Questions and Answer related to Strength of Materials

What is engineering stress?

Instantaneous load or force applied per unit original area of cross-section (Before any application of force) is known as engineering stress.

It is denoted by σ (sigma). SI unit of engineering stress is N/m2 or Pascal (Pa).

What is Engineering Strain?

Change in length at some instant of the material per unit original length (Before any application of force) is known as engineering strain.

It is denoted by ε (Epsilon) or γ (Gamma). It’s a unitless quantity.

What is Tensile Stress?

When the applied force is away from the material, then the Stress produced is known as tensile stress.

Strength of Materials : Tensile Stress Figure
Strength of Materials : Tensile Stress

What is Compressive Stress?

When the applied force is in towards the object, then the Stress produced is known as compressive stress.

new image
Strength of Materials : Compressive Stress

What is Shear Stress?

When the applied force is parallel to the area on which it is applied, the Stress is known as shear stress.

What is Factor of Safety?

There are always some uncertainties in the measured values of stresses; therefore, the stress that we are going to consider for our use known as working Stress (σw) is always less than the experimental value of Stress. In most of the applications, we consider yield strength (σy).

Working Stress is determined by reducing the yield strength by a factor; that factor is known as the factor of safety. So, the factor of safety is a ratio of yield strength to working stress. Its symbol is N. It is a unitless quantity.

What is True Stress-Strain Curve?

It is a stress-strain curve in which true Stress is plotted against true strain. Both Stress and strain are based on instantaneous measurement hence instantaneous area of the cross-section is considered instead of original cross-section and instantaneous length is considered instead of the original length.

What is Breaking Point?

Stress necessary to continue plastic deformation starts to decrease after ultimate strength and eventually breaks the material at a point known as breaking point.

What is Ultimate Tensile Strength?

After yielding, as plastic deformation continues, it reaches a maximum limit known as ultimate Stress or ultimate strength, it is also known as Ultimate Tensile Strength (UTS)

What is Hooke’s Law? | Explain Hooke’s Law

When this type of deformation occurs, the strain in the metal piece is nearly proportional to the stress; therefore, this deformation occurs as a straight line in Stress versus strain plot except for some materials like grey cast iron, concrete and many polymers. Stress is proportional to the strain through this relationship.

e9 1

This is known as Hooke’s Law, where Y the proportionality constant is known as Young’s Modulus.

It is one of the most important law in the studies of Strength of Materials.

CONCLUSION

In this articles important terminology of strength of materials are explained in detailed such as engineering stress, strain, stress-strain curve for both ductile and brittle materials, young modulus, Poisson’s ratio etc. Strength of materials is also known as mechanics of materials.

To Learn more on mechanical engineering and Strength of Materials click here!