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Question: A bimetallic strip is formed out of two identical strips, one of copper and the other of brass. the ...

A bimetallic strip is formed out of two identical strips, one of copper and the other of brass. the coefficients of linear expansion of the two metals are αc{{\alpha }_{c}}and αb{{\alpha }_{b}}(αb>αc{{\alpha }_{b}}>{{\alpha }_{c}}). On heating the bimetallic strip through temperature ΔT\Delta T, the strip bends into an arc of a circle. find the radius of curvature of the strip
A. R=2d(αbαc)ΔTR=\dfrac{2d}{\left( {{\alpha }_{b}}-{{\alpha }_{c}} \right)\Delta T}
B. R=3d(αbαc)ΔTR=\dfrac{3d}{({{\alpha }_{b}}-{{\alpha }_{c}})\Delta T}
C. R=d(αbαc)ΔTR=\dfrac{d}{({{\alpha }_{b}}-{{\alpha }_{c}})\Delta T}
D. R=d2(αbαc)ΔTR=\dfrac{d}{2({{\alpha }_{b}}-{{\alpha }_{c}})\Delta T}

Explanation

Solution

Bimetallic strips are strips consisting of two different metals having different temperature coefficients. They expand or contract whenever there is change in temperature. Their expansion is governed by a basic law.

Formula used:
l=l0(1+αΔT)l={{l}_{0}}(1+\alpha \Delta T)
l=Rθl=R\theta

Complete step by step answer:
Let us consider a strip as described in the question. Let the first layer of the bimetallic strip be of copper and the second layer on the bimetallic strip be of brass. Also, consider the width of the bimetallic strip be dd.
As we heat the bimetallic strip, it heats up, bends and gets formed into the shape of an arc as shown in the figure.

Let the arc formed be a part of a circle with radius RR
As we know, for a given material, it can be written as
l=l0(1+αΔT)l={{l}_{0}}(1+\alpha \Delta T)
Here, the initial length of both the copper and brass layers is the same. Let it be l0{{l}_{0}}
Thus, for copper strip: lc=l0(1+αcΔT){{l}_{c}}={{l}_{0}}(1+{{\alpha }_{c}}\Delta T) ---(i)
For brass strip: lb=l0(1+αbΔT){{l}_{b}}={{l}_{0}}(1+{{\alpha }_{b}}\Delta T) ---(ii)
Also, as they are a part of the arc of a circle, we can say that
Arc length = Radius * angle subtended
Thus, for copper:
lc=Rθ{{l}_{c}}=R\theta ----(iii)
And for brass:
lb=(R+d)θ{{l}_{b}}=\left( R+d \right)\theta ----(iv)
From equation (i) and (iii)
Rθ=l0(1+αcΔT)R\theta ={{l}_{0}}(1+{{\alpha }_{c}}\Delta T) ----(v)
Also, from equation (ii) and (iv)
(R+d)θ=l0(1+αbΔT)(R+d)\theta ={{l}_{0}}(1+{{\alpha }_{b}}\Delta T) ----(vi)
Now, (vi)/ (v):
(R+d)θRθ=l0(1+αbΔT)l0(1+αcΔT)\dfrac{(R+d)\theta }{R\theta }=\dfrac{{{l}_{0}}(1+{{\alpha }_{b}}\Delta T)}{{{l}_{0}}(1+{{\alpha }_{c}}\Delta T)}
(R+d)R=(1+αbΔT)(1+αcΔT)1\Rightarrow \dfrac{(R+d)}{R}=(1+{{\alpha }_{b}}\Delta T){{(1+{{\alpha }_{c}}\Delta T)}^{-1}}
Using Binomial theorem, (1+at)1=1at{{(1+at)}^{-1}}=1-at
Here, we get:
(R+d)R=(1+αbΔT)(1αcΔT)\Rightarrow \dfrac{(R+d)}{R}=(1+{{\alpha }_{b}}\Delta T)(1-{{\alpha }_{c}}\Delta T)
1+dR=1+(αbαc)ΔT+ΔT2\Rightarrow 1+\dfrac{d}{R}=1+({{\alpha }_{b}}-{{\alpha }_{c}})\Delta T+\Delta {{T}^{2}}
Here, ΔT2very very small\Delta {{T}^{2}}\to \text{very very small}
So, we neglect it.
dR=(αbαc)ΔT\Rightarrow \dfrac{d}{R}=({{\alpha }_{b}}-{{\alpha }_{c}})\Delta T
R=d(αbαc)ΔT\Rightarrow R=\dfrac{d}{({{\alpha }_{b}}-{{\alpha }_{c}})\Delta T}
Thus, the correct option is (c).

Note:
Bimetallic strips are predominantly used in some thermostats to measure the change in temperature. Due to the presence of two different metals, they expand or contract at different rates causing the strip to bend. This bend indicates change in temperature.