Change Of Resistance In Wires By Stretching

Change Of Resistance In Wires By Stretching

Vishal kumarUpdated on 02 Jul 2025, 05:51 PM IST

The resistance of a wire changes when it is stretched, a phenomenon that is directly related to the wire's physical dimensions and the material's properties. As a wire is stretched, its length increases and its cross-sectional area decreases, leading to an increase in resistance. This concept is important in various applications, such as in strain gauges, where the change in resistance due to stretching is used to measure mechanical strain. In everyday life, understanding how stretching affects resistance can help in designing and maintaining electrical systems, ensuring that wires function safely and efficiently under different mechanical stresses. This article discusses the principles behind the change in resistance due to stretching, the mathematical relationship governing this change, and some solved examples based on this concept.

This Story also Contains

  1. Stretching of wire
  2. Solved Examples Based on Change Of Resistance In Wires By Stretching
  3. Summary
Change Of Resistance In Wires By Stretching
Change Of Resistance In Wires By Stretching

Stretching of wire

If a conducting wire stretches its length increases area of cross-section decreases but the volume remains constant

Suppose for a conducting wire before stretching

it's length $=l_1$, area of cross-section $=A_{1, \text { radius }}=r_1$, diameter $=d_1$, and resistance $R_1=\rho \frac{l_1}{A_1}$

After stretching length $=l_2$, area of cross-section $=A_{2, \text { radius }}=r_2$, diameter $=d_2$
$
\begin{aligned}
& \text { and resistance } R_2=\rho \frac{l_2}{A_2} \\
& \qquad \frac{R_1}{R_2}=\frac{l_1}{l_2} * \frac{A_2}{A_1}
\end{aligned}
$

But Volume is constant So

$\begin{aligned} & A_1 l_1=A_2 l_2 \\ & \Rightarrow \frac{l_1}{l_2}=\frac{A_1}{A_2} \\ & \text { Now } \\ & \frac{R_1}{R_2}=\frac{l_1}{l_2} * \frac{A_2}{A_1}=\left(\frac{l_1}{l_2}\right)^2=\left(\frac{A_2}{A_1}\right)^2=\left(\frac{r_2}{r_1}\right)^4=\left(\frac{d_2}{d_1}\right)^4\end{aligned}$

If a wire of resistance $R$ and length I is stretched to length nl, then the new resistance of a wire is $n^2 R$

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Solved Examples Based on Change Of Resistance In Wires By Stretching

Example 1: If a wire is stretched to make it 0.1% longer, its resistance will

1) increase by $0.05 \%$
2) increase by $0.2 \%$
3) decrease by $0.2 \%$
4) decrease by $0.05 \%$

Solution:

Ratio of resistances

If length is given

$R \alpha l^2$
wherein
$
\begin{aligned}
& \frac{R_1}{R_2}=\left(\frac{l_1}{l_2}\right)^2 \\
& \quad l A=\text { constant } \\
& A=\frac{K}{l} \\
& R=\frac{\rho l}{A}=\rho \frac{l}{K / l}=\frac{\rho}{K} l^2 \\
& \quad l=l_0+(0.001 l) \\
& R^{\prime}=\frac{\rho}{K} l_0^2[1+0.001]^2=R_0[1+0.002]
\end{aligned}
$

Hence, the answer is option (3).

Example 2: A copper wire is stretched to make it 0.5 % longer. The percentage change (in %) in its electrical resistance if its volume remains unchanged is :

1) 1

2) 2.5

3) 2

4) 0.5

Solution:

Stretching of wire

If a conducting wire stretches its length increases area of cross-section decreases but the volume remains constant

Since Volume is constant

Let the initial area of the wire be A, the length be L and the resistance be R

$\begin{aligned} & \therefore V=A . l \text { and } R=\frac{\rho l}{A} \\ & \mathrm{~A} . \mathrm{l}=\mathrm{A}_1(1+0.0051) \\ & A_1=\frac{A}{1.005} \\ & R_1=\frac{\rho(1.005) l}{\frac{A}{1.005}}=R(1.005)^2=1.01 R \\ & \text { percentage change } \\ & =\frac{(1.01-1) l}{1} \times 100=1 \%\end{aligned}$

Hence, the answer is the option (1).

Example 3: A metal wire having resistance R, stretched in such a way that its radius becomes half. The new value of resistance is

1) 16R

2) R/16

3) 4R

4) R/4

Solution:

If you stretch the wire till its radius is halved by the previous value, then its length will increase 4 times to keep the volume constant.

Resistivity remains the same as it depends upon the material of the wire.

So, the new resistance will be 16 times.

Hence, the answer is the option 1.

Example 4: A wire of $1 \Omega$ has a length of 1 m . It is stretched till its length increases by 25\%. The percentage change in resistance to the nearest integer is:
1) $25 \%$
2) $76 \%$
3) $12.5 \%$
4) $56 \%$

Solution:

As volume of wire remains constant so
$
\mathrm{A}_0 \ell_0=\mathrm{A}_1 \ell_1 \Rightarrow \mathrm{A}_1=\frac{\ell_0 \mathrm{~A}_0}{\ell_1}
$

Now
$
\begin{aligned}
& \text { Resistance }(\mathrm{R})=\frac{\rho \ell}{\mathrm{A}} \\
& \frac{\mathrm{R}_0}{\mathrm{R}_1}=\frac{\rho \ell_0 / \mathrm{A}_0}{\rho \ell_1 / \mathrm{A}_1} \\
& \frac{1}{\mathrm{R}_1}=\frac{\ell_0}{\mathrm{~A}_0}\left(\frac{\ell_0 \mathrm{~A}_0}{\ell_1 \times \ell_1}\right) \mathrm{R}_1=\frac{\ell_1^2}{\ell_0^2}=1.5625 \Omega
\end{aligned}
$

So \% change in resistance
$
\begin{aligned}
& =\frac{R_1-R_0}{R_0} \times 100 \% \\
& =\frac{1.5625-1}{1} \times 100 \% \\
& =56.25 \%
\end{aligned}
$

Hence, the answer is the option (4).

Example 5: A copper wire is stretched to make it 0.1 % longer. The percentage change in its resistance is:

1) 0.2 % increase

2) 0.2% decrease

3) 0.1 % increase

4) 0.1 % decrease

Solution:

For the stretched wire, $R \alpha l^2$
For a small change in the length, we can write $\frac{\Delta R}{R}=2 \frac{\Delta l}{l}$
Percentage change in the resistance $=\frac{\Delta R}{R} \times 100=2 \frac{\Delta l}{l} \times 100=0.2 \%$
Hence, the answer is the option (1).

Summary

When a wire is elongated, its resistance changes due to modifications in its physical dimensions. The wire becomes longer and thinner when extended. According to the formula $R=\rho \frac{L}{A}$ (where R is resistance, $\rho$ is resistivity, L is length, and A is cross-sectional area), increasing the length $L$ and decreasing the area $A$ result in a higher resistance.

Frequently Asked Questions (FAQs)

Q: What is the relationship between localization length and resistance changes in disordered stretched wires?
A:
The localization length describes the spatial extent of electron wavefunctions in disordered systems. In disordered wires, stretching can alter the degree of disorder and thus the localization length. If stretching reduces the localization length to less than the wire length, it can lead to a transition from metallic to insulating behavior, dramatically changing the resistance.
Q: How does the concept of ballistic transport apply to resistance changes in extremely short stretched wires?
A:
In extremely short wires where the length is less than the electron mean free path, transport becomes ballistic rather than diffusive. Stretching such wires can change the probability of electrons traversing the wire without scattering, leading to resistance changes that don't follow classical expectations and may exhibit quantum mechanical effects.
Q: Can spin-orbit coupling effects contribute to resistance changes in stretched magnetic nanowires?
A:
Yes, spin-orbit coupling, which links an electron's spin to its orbital motion, can be affected by mechanical strain. In magnetic nanowires, stretching can alter the strength of spin-orbit coupling, potentially leading to changes in magnetoresistance. This effect adds another dimension to understanding resistance changes in these specialized materials.
Q: What is the significance of the Burger's vector in understanding resistance changes of stretched crystalline wires?
A:
The Burger's vector describes the magnitude and direction of lattice distortion associated with dislocations in crystalline materials. When a crystalline wire is stretched, the movement and multiplication of dislocations, characterized by their Burger's vectors, can affect electron scattering and thus contribute to resistance changes.
Q: How does the concept of electron mean free path relate to resistance changes in stretched nanowires?
A:
The electron mean free path is the average distance an electron travels between collisions. In nanowires, where dimensions can be comparable to this length, stretching can significantly alter the mean free path. This can lead to resistance changes that are more pronounced and complex than in larger wires, where the mean free path is much shorter than the wire dimensions.
Q: Can thermoelectric effects influence resistance measurements in stretched wires?
A:
Yes, thermoelectric effects like the Seebeck effect can influence resistance measurements, especially if temperature gradients are present. Stretching a wire can create such gradients due to the thermoelastic effect, potentially leading to small voltages that could be misinterpreted as resistance changes if not accounted for.
Q: What is the relationship between Hooke's law and resistance changes in stretched wires within the elastic limit?
A:
Hooke's law states that strain is proportional to stress within the elastic limit. For wires obeying Hooke's law, the dimensional changes (and thus resistance changes) are proportional to the applied force. This linear relationship simplifies the prediction and analysis of resistance changes in the elastic region.
Q: How does the concept of strain energy relate to resistance changes in stretched wires?
A:
Strain energy is the potential energy stored in a material as it is deformed. In stretched wires, this energy is related to the work done in stretching. The amount of strain energy can correlate with the degree of atomic displacement and lattice distortion, which in turn can affect the wire's resistance.
Q: Can magnetostriction affect resistance changes in stretched ferromagnetic wires?
A:
Yes, magnetostriction - the change in a material's dimensions in response to a magnetic field - can interact with mechanical stretching in ferromagnetic wires. This interaction can lead to complex relationships between applied stress, magnetic fields, and resistance changes, particularly important in sensing applications.
Q: How do surface effects contribute to resistance changes in very thin stretched wires?
A:
In very thin wires, the surface-to-volume ratio is high, making surface effects more prominent. Stretching can alter surface roughness and the distribution of surface defects, significantly affecting electron scattering at the surface. This can lead to resistance changes that are more pronounced than in thicker wires.