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Question: Calculate the diameter of the brass wire.![](https://www.vedantu.com/question-sets/822838e5-ea18-433...

Calculate the diameter of the brass wire.

A. 2.1×104m2.1 \times {10^{ - 4}}m
B. 4.2×104m4.2 \times {10^{ - 4}}m
C. 8.4×104m8.4 \times {10^{ - 4}}m
D. 16.8×104m16.8 \times {10^{ - 4}}m

Explanation

Solution

Correction if the question calculates the diameter of brass wire. Given diameter of steel wire is 0.6mm0.6mm and ybys=12\dfrac{{{y_b}}}{{{y_s}}} = \dfrac{1}{2} . Since the weight AB are equally distributed in both wires, the strain will be the same in both i.e. ratio of stress to young's modulus of elasticity will be constant.
(1) StressYoungs modules=constant\dfrac{{Stress}}{{Young's{\text{ modules}}}} = cons\tan t
(2) Area of base of wire =πr2 = \pi {r^2}
Where r is the radius of base.

Complete step by step answer:
Since both the wires i.e. steel and brass are subjected to weight AB this weight will produce elongation in the wire.
The ratio of longitudinal stress as the longitudinal strain within the elastic limit is known as young’s modulus of elasticity, Y.
Now, as the weight is equally distributed on both wires, so the strain in both the wires will be the same.
Now, young’s modulus, Y=StressStrainY = \dfrac{{Stress}}{{Strain}}
StressY=Strain\Rightarrow \dfrac{{Stress}}{Y} = Strain
As strain is same, it can be treated constant here
So, StressY=Constant\dfrac{{Stress}}{Y} = Cons\tan t
(StressY)brass=(StressY)steel\Rightarrow {\left( {\dfrac{{Stress}}{Y}} \right)_{brass}} = {\left( {\dfrac{{Stress}}{Y}} \right)_{steel}}…. (i)
Now, stress =ForceArea = \dfrac{{Force}}{{Area}}
And, Area =πr2 = \pi {r^2}… (Where r is radius of wire)
So, stress =Forceπr2 = \dfrac{{Force}}{{\pi {r^2}}}
Also, since weights are equally distributed, force will also be the same in both.
So, equation (i) become
Force(Area)brass×Yb=Force(Area)steel×Ys 1πrb2×Yb=1πrs2×Ys  \dfrac{{Force}}{{{{\left( {Area} \right)}_{brass}} \times {Y_b}}} = \dfrac{{Force}}{{{{\left( {Area} \right)}_{steel}} \times {Y_s}}} \\\ \Rightarrow \dfrac{1}{{\pi r_b^2 \times {Y_b}}} = \dfrac{1}{{\pi r_s^2 \times {Y_s}}} \\\
Where, Yb{Y_b} is young’s modulus for brass and Ys{Y_s} is young’s modulus for steel
Also, rb{r_b} is radius of brass and rs{r_s} is radius of steel =0.62=0.3m = \dfrac{{0.6}}{2} = 0.3m
=0.3×103= 0.3 \times {10^{ - 3}}
1rb2×Yb=1rs2×Ys 1rb2=YbYs×1rs2 1rb2=12×1(0.3×103)2 rb=2×(0.3×103)2 rb=1.414×0.3×103=0.424m×103  \Rightarrow \dfrac{1}{{r_b^2 \times {Y_b}}} = \dfrac{1}{{r_s^2 \times {Y_s}}} \\\ \Rightarrow \dfrac{1}{{r_b^2}} = \dfrac{{{Y_b}}}{{{Y_s}}} \times \dfrac{1}{{r_s^2}} \\\ \Rightarrow \dfrac{1}{{r_b^2}} = \dfrac{1}{2} \times \dfrac{1}{{{{\left( {0.3 \times {{10}^{ - 3}}} \right)}^2}}} \\\ \Rightarrow r_b^{} = \sqrt {2 \times {{\left( {0.3 \times {{10}^{ - 3}}} \right)}^2}} \\\ \Rightarrow {r_b} = 1.414 \times 0.3 \times {10^{ - 3}} = 0.424m \times {10^{ - 3}} \\\
So, diameter of brass =2×0.4242×103 = 2 \times 0.4242 \times {10^{ - 3}}
=0.8484×103= 0.8484 \times {10^{ - 3}}
=8.4×104m= 8.4 \times {10^{ - 4}}m

So, the correct answer is “Option C”.

Note:
Here Area=πr2Area = {\pi r^2} because the area is to be taken where the force acts. As the force acts on the base of wire. So, the area of the base which is circular in shape is taken.