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Question: The resistance of a wire at room temperature \[{30^\circ }C\] is found to be \[10\Omega \] . Now to ...

The resistance of a wire at room temperature 30C{30^\circ }C is found to be 10Ω10\Omega . Now to increase the resistance by 10%10\% , the temperature of the wire must be: [The temperature coefficient of resistance of the material of the wire is 0.002 per Celsius]
(A) 36C{36^\circ }C
(B) 83C{83^\circ }C
(C) 63C{63^\circ }C
(D) 33C{33^\circ }C

Explanation

Solution

Hint In this question, we are given the initial conditions of the wire. We know that when a wire is heated, it experiences gain in resistance. This gain in resistance should be equal to 10%10\% . We can also infer that if the original resistance was R, the new resistance should be 1.1R.
Use the following relation
RT=R0(1+αT){R_T} = {R_0}(1 + \alpha T)

Complete step by step solution
According to the question
Temperature coefficient of resistance of the wire,
α=0.002/C\alpha = 0.002{/^\circ }C
Resistance at temperature,
30C=R30=10Ω{30^\circ }C = {R_{30}} = 10\Omega
We know,
RT=R0(1+αT){R_T} = {R_0}(1 + \alpha T)
Putting the value of R30{R_{30}} , α\alpha and T in above equation we have
10=R0(1+30α)10 = {R_0}(1 + 30\alpha ) … (i)
After 10%10\% increase in resistance the new resistance becomes
10+10×10100=11Ω10 + 10 \times \dfrac{{10}}{{100}} = 11\Omega
Again, for the new resistance we have
11=R0(1+αT)11 = {R_0}(1 + \alpha T) … (ii)
Dividing equation (ii) by (i), we get
1110=R0(1+αT)R0(1+30α)\dfrac{{11}}{{10}} = \dfrac{{{R_0}(1 + \alpha T)}}{{{R_0}(1 + 30\alpha )}}
R0{R_0} gets cancelled out as it’s the same material and same reference temperature.
Or, 1110=(1+αT)(1+30α)\dfrac{{11}}{{10}} = \dfrac{{(1 + \alpha T)}}{{(1 + 30\alpha )}}
Or, 11(1+30α)=10(1+αT)11(1 + 30\alpha ) = 10(1 + \alpha T)
Or, 11+330α=10+10αT11 + 330\alpha = 10 + 10\alpha T
Or, 1+330α=10αT1 + 330\alpha = 10\alpha T
Or, 1+330α10α=T\dfrac{{1 + 330\alpha }}{{10\alpha }} = T
Putting the value of α\alpha , we get
T=1+330×0.00210×0.002T = \dfrac{{1 + 330 \times 0.002}}{{10 \times 0.002}}
Or, T=83CT = {83^ \circ }C (Option B)
Option B is correct answer

Note The above calculation is made with the consideration that the reference temperature is the same. Although in case of different reference temperature the above formula becomes,
RT=R0(1+α(TT0)){R_T} = {R_0}(1 + \alpha (T - {T_0}))
Where, RT{R_T} = Conductor resistance at temperature “T”.
R0{R_0} = Conductor resistance at reference temperature.
α\alpha = Temperature coefficient of resistance of the material of the conductor.
T = Conductor temperature in degree Celsius.
R0{R_0} = Reference temperature in degree Celsius.
Resistance of a conductor increases with the increasing temperature because the chance of electrons colliding with protons increases. Resistance decreases with decreasing temperature. However, in some cases when the temperature is decreased beyond a critical temperature its resistance becomes zero, such materials are called superconductors. The critical temperature for mercury is 4.15 K.