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What Is Longitudinal Strain in Physics?

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Formula, Examples, and Applications of Longitudinal Strain

Stress and strain are two sides of a coin. A very common example among physics enthusiasts, while they are explaining this topic, is to tell students that the stress being referred to here is not the one that students face in their exams. We will not be using this example because we fully understand that students are capable and smart enough to figure that out on their own. Stress in terms of Physics is the force acting on a unit area of a material. The strain, on the other hand, is just a basic measure that gives us an idea of how much an object has deformed or changed due to the stress applied to it. This is the main idea behind the concept of stress and strain.


Longitudinal strain is a very interesting and simple topic that is very easy to understand. This topic literally guarantees marks as students do not really have to spend a lot of time on the understanding part of it because of its simplicity. Plus questions from the topic keep appearing in class 12 School level examinations and even competitive exams like JEE and NEET. In order to secure these marks which can be obtained by simply understanding the topic, we recommend students to read this article thoroughly and throughout. Only then will they be able to understand the chapter fully and figure out what the concept is about.


Vedantu offers nothing but the best quality articles when it comes to testing preparation. This is the same goal behind this article as well and that is why we plan on giving you the best resource on the topic of longitudinal strain that can be understood with ease at the comfort of your home, school or anywhere. 


Strain is the force inclined to pull or stretch something to an extreme or damaging degree.


When an external force per unit area (stress) is applied to an object, and there is a deformity in its shape. 


The inter-atomic particles inside the body try to regain its original position. While the body exceeds the elastic limit.


Such a condition where the internal restoration force fails to bring the body back to its original shape and this condition is called the strain.


The property of strain is that the elastic strain is irreversible.


SI Unit of Strain

In Mechanics, strain is often said to be “dimensionless” regardless of what system we use as it has no units.


Strain  = Change in length / original length


Δ L/ L  =   \ \[\left [ L^{1}\right ]\]/ \[\left [ L^{1}\right ]\]=   \[\left [ L^{0}\right ]\] = 1


If we use meters/ meters. It will always come as 1.


So,


    SI unit of strain  =  one (no unit)


Unit of Strain

The unit of strain in non-SI units,


Other units of strain = cm/cm or cubits/ cubits will always give 1.


Unit of strain = 1 (no unit)


Generally, we identify a number as strain.


We generally use the strain after the number such as 0.012 strain.


The measurement of strain is usually given as the numeric units in (με).


Since the changes in length are usually very small and a typical strain measurement in the English system is given as microinches per inch (i.e., in the order of 10−6


Therefore, the numeric value, which is unitless, will remain the same in any system.


Longitudinal Strain Definition

The longitudinal strain is defined as the ratio of change in length of the material due to the applied force to the original length.


Longitudinal Strain

When stress (external force per unit area) is applied on the body such that this deforming force causes a change in the length alone, and the body exceeds its elastic limit. This condition or strain produced in the body is called the longitudinal strain.


As the name longitudinal strain suggests that we are talking about the length and strain is causing deformity in its shape by elongating its length.


(Image will be uploaded soon)


In Fig.1, a rod of length ‘Lo’ is stretched along the X-axis with enough external force that its length is extended to ‘Δ L’.


Now, the new length of the rod is Lf, which equals Lo + Δ L.


 Δ L is the extended length of the rod.


This has happened due to the strain in the rod.


Longitudinal strain is denoted by a Greek symbol epsilon, ε


So, the formula for the longitudinal strain is given by,


ε =   Change in length/ original length  =  = Lf- Lo/ Lo  = Δ L/ L


The unit of longitudinal strain is one.


The dimensional formula =\[\left [ L^{0}\right ]\]


Young’s Modulus of Elasticity (γ) 

For a given material there can be different types of modulus of elasticity depending upon the type of stress applied, and the resulting strain produced. One of them is young’s modulus of elasticity. Young’s modulus of elasticity corresponds to the ratio of longitudinal stress to the longitudinal strain within the elastic limit. 


Consider a wire PQ (in  Fig.2) of length L of the radius of cross-section, ‘r’ and uniform cross-sectional area ‘A’ is suspended from a rigid support P. When stretched by a suspended load of ‘mg’ from the other end Q.


(The image will be uploaded soon)


Therefore, a force (perpendicular force) F is applied at its free end. Such that there is an elongation in the body by Δ L.


Young’s modulus or γ = Longitudinal stress/ longitudinal strain…(1)


Where,


Longitudinal stress is the deforming force when applied to the body, the stress is produced in the body causing elongation in its length.


Its formula is the same as the stress which is equal to F/A (Force per unit area)


       Longitudinal stress = \[\frac{F}{A}\] = \[\frac{F}{\Pi r^{2}}\] …. (2)


and, longitudinal strain  =  Δ L/ L..(3)


So,  putting values of (2) and (3)  in (1) 


=  F/πr²/  Δ L/ L 


Longitudinal Strain


γ = \[\frac{F.L}{\Pi r^{2}}\] . Δ L

  • Within the elastic limit, this ratio always remains constant.

  • The unit of γ  in SI is N/m² or Pascal (Pa).

  • In CGS system = dyne/cm²

  • The dimensional formula for γ is \[\left [ M^{1} L^{-1}T^{-2}\right ]\]


Key Point

If the length increases from its natural length, the longitudinal strain is called the tensile strain and if the length decreases from its natural or original length, then it is the compression strain.


Do You Know?

  • In a suspension bridge, there is a stretch in the ropes by the load because of which length of rope varies. Hence young’s modulus of elasticity is involved in real life.


Conclusion 

We hope that this article was able to solve all your doubts about the concept of longitudinal strain. The idea behind stress and strain is not all that complex but is very easy to understand and comprehend. We suggest that students go through this article again and again to get a complete idea of what the entire concept is about. Vedantu has been a leader in the world of education because we believe in the power of good and easy to understand resources for students of all ages. It is due to the same reason that we have had so many success stories of students from around the world and across the country as they score well in their exams. This article was written with the same intention. The intention was to offer nothing but the best and the easiest to understand study document that can be studied anywhere by students on any device that they own. Vedantu hopes that we were able to solve all the doubts that you had about the topic.

FAQs on What Is Longitudinal Strain in Physics?

1. What is longitudinal strain in Physics?

In Physics, longitudinal strain is defined as the measure of deformation that occurs in an object along the direction of an applied force. It is calculated as the ratio of the change in the object's length (ΔL) to its original length (L). It essentially quantifies how much an object stretches or compresses relative to its initial size when a force is applied along its axis.

2. What is the formula for calculating longitudinal strain, and what are its SI units?

The formula for longitudinal strain (often denoted by the Greek letter epsilon, ε) is:

Longitudinal Strain (ε) = Change in Length (ΔL) / Original Length (L)

Since it is a ratio of two lengths (e.g., meters divided by meters), the units cancel out. Therefore, longitudinal strain is a dimensionless quantity and has no units.

3. What are the main types of longitudinal strain?

Longitudinal strain can be classified into two main types based on the nature of the deforming force:

  • Tensile Strain: This occurs when an object is stretched by a pulling force (tensile force), resulting in an increase in its length. For example, stretching a rubber band.

  • Compressive Strain: This occurs when an object is compressed by a pushing force (compressive force), resulting in a decrease in its length. For example, the compression of a concrete pillar under the weight of a building.

4. How does longitudinal strain differ from longitudinal stress?

Longitudinal strain and longitudinal stress are related but distinct concepts that describe a material's response to force. Here’s the key difference:

  • Focus: Stress is the internal restoring force per unit area that a material exerts to resist deformation. Strain is the measure of the actual physical deformation (the fractional change in length) that occurs.

  • Cause and Effect: Stress is the cause, while strain is the effect. Applying a stress to a body causes it to experience strain.

  • Units: Stress is measured in Pascals (N/m²), whereas strain is a unitless ratio.

5. What is the importance of studying longitudinal strain?

Studying longitudinal strain is crucial in engineering and materials science because it helps predict how materials will behave under load. By understanding a material's strain response, engineers can design structures like bridges, buildings, and aircraft components that can safely withstand forces without deforming excessively or breaking. It is a fundamental property for determining a material's elasticity and strength.

6. Can you explain the difference between longitudinal, lateral, and volumetric strain?

Yes, these three types of strain describe deformation in different dimensions:

  • Longitudinal Strain: Measures the change in length per unit length along the axis of the applied force.

  • Lateral Strain: Measures the change in dimensions (like diameter or width) per unit dimension perpendicular to the axis of the applied force. For instance, when you stretch a wire, its length increases (longitudinal strain), but its diameter decreases (lateral strain).

  • Volumetric Strain: Measures the change in the overall volume of an object per unit of its original volume, typically caused by pressure from all sides.

7. Why is strain a more useful measure of deformation than the absolute change in length (ΔL)?

The absolute change in length (ΔL) is dependent on the object's initial size. For example, a 1 cm stretch in a 10 cm wire is very significant, but the same 1 cm stretch in a 1 km long cable is negligible. Strain (ΔL/L) is a ratio that normalises this deformation, making it an intrinsic property that describes how the material itself deforms, regardless of the object's original dimensions. This allows engineers to compare the properties of materials fairly.

8. What is Poisson's Ratio and how does it connect lateral and longitudinal strain?

Poisson's Ratio is a fundamental material property that describes the relationship between lateral and longitudinal strain. It is defined as the negative ratio of the lateral strain to the longitudinal strain. Essentially, it quantifies how much a material tends to narrow in cross-section when it is stretched. A material with a high Poisson's ratio becomes significantly thinner when pulled.