The Young’s modulus is defined as the ratio of stress to strain in a material and is a measure of the stiffness of the material. It is a property that is intrinsic to the material and does not depend on the dimensions of the material's shape or size.
Let's dive into the problem:
The Young's modulus \( Y \) is given by:
\(Y = \frac{F/A}{\Delta L/L}\)
Where:
Now, let's consider the changes in the wire:
The new cross-sectional area \(A'\) becomes:
\(A' = \pi (r')^2 = \pi \left(\frac{r}{2}\right)^2 = \frac{\pi r^2}{4} = \frac{A}{4}\)
At this point, it is essential to remember that Young's modulus is a material property and does not depend on the material’s dimensions or shape. Thus, regardless of changes in length or cross-sectional area, the intrinsic stiffness or Young’s modulus of the material remains the same.
Consequently, the correct answer is:
Remain same
A steel wire of length 4.7 m and cross-sectional area 3.0 × 10-5 m2 stretches by the same amount as a copper wire of length 3.5 m and cross-sectional area of 4.0 × 10–5 m2 under a given load. What is the ratio of the Young’s modulus of steel to that of copper?
Two wires of diameter 0.25 cm, one made of steel and the other made of brass are loaded as shown in Fig. 8.11. The unloaded length of steel wire is 1.5 m and that of brass wire is 1.0 m. Compute the elongations of the steel and the brass wires.

Read the following two statements below carefully and state, with reasons, if it is true or false.
(a) The Young’s modulus of rubber is greater than that of steel;
(b) The stretching of a coil is determined by its shear modulus.