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Question: The temperature coefficient of resistance of a wire is 0.00125 per degree Celsius. At 300K its resis...

The temperature coefficient of resistance of a wire is 0.00125 per degree Celsius. At 300K its resistance is 1 ohm. The resistance of the wire will be 2 ohms at the following temperature:

A) 1127 K

B) 400K

C) 600K

D) 1400K

Explanation

Solution

Resistance of any substance is linearly proportional to the absolute temperature of that substance. The proportionality coefficient is known as the temperature coefficient of that particular substance and the value of that coefficient varies from substance to substance.

Formula used:

The relationship between resistance and its absolute temperature is:

RT=R0(1+αΔT){R_T} = {R_0}\left( {1 + \alpha \Delta T} \right) ……………..(1)

Where,

RT{R_T} is the resistance at absolute temperature TT,

R0{R_0} is the resistance at reference temperature,

α\alpha is the temperature coefficient of resistance for the substance,

ΔT\Delta T is the temperature difference between reference and T.

Complete step by step solution:

Given:

The temperature coefficient of the wire is α=0.00125/C\alpha = 0.00125{/^ \circ }C

Temperature of the wire is T1=300K=27oC{T_1} = 300K = 27 ^oC.

Resistance of the wire at 300K300K is RT1=1Ω{R_{{T_1}}} = 1\Omega .

Later, resistance of the wire at T2{T_2} will be RT2=2Ω{R_{{T_2}}} = 2\Omega .

To find: The temperature of T2{T_2} when the resistance of the wire will be 2 Ohm.

Step 1:

Using eq.(1) take the ratio of two resistance at two different temperatures T1{T_1} and T2{T_2}, then find an expression to get the value of T2{T_2} as:

0oC0 ^oC is the reference temperature.

ΔT  for  1Ω=(T10)=T1\Delta T\;for\;1\Omega = (T_1 - 0) = T_1

ΔT  for  2Ω=(T20)=T2\Delta T\;for\;2\Omega = (T_2 - 0) = T_2

RT2RT1=R0(1+αT2)R0(1+αT1)\dfrac{{{R_{{T_2}}}}}{{{R_{{T_1}}}}} = \dfrac{{{R_0}\left( {1 + \alpha {T_2}} \right)}}{{{R_0}\left( {1 + \alpha {T_1}} \right)}}

RT2+αT1RT2=RT1+αT2RT1\Rightarrow {R_{{T_2}}} + \alpha {T_1}{R_{{T_2}}} = {R_{{T_1}}} + \alpha {T_2}{R_{{T_1}}}

αT2RT1=(RT2RT1)+αT1RT2\Rightarrow \alpha {T_2}{R_{{T_1}}} = ({R_{{T_2}}} - {R_{{T_1}}}) + \alpha {T_1}{R_{{T_2}}}

T2=(RT2RT1)αRT1+T1RT2RT1\therefore {T_2} = \dfrac{{({R_{{T_2}}} - {R_{{T_1}}})}}{{\alpha {R_{{T_1}}}}} + \dfrac{{{T_1}{R_{{T_2}}}}}{{{R_{{T_1}}}}}………………. (2)

Step 2:

Now, substitute the values of α\alpha , T1{T_1}, RT1{R_{{T_1}}}, RT2{R_{{T_2}}} in eq.(2) to get the value of T2{T_2} as:

T2=(21)Ω0.00125C1×1Ω+27×2Ω1Ω{T_2} = \dfrac{{\left( {2 - 1} \right)\Omega }}{{0.00125{C^{ - 1}} \times 1\Omega }} + \dfrac{{27 \times 2\Omega }}{{1\Omega }}

T2=10.00125+54=800+54=854oC=854+273=1127K\therefore {T_2} = \dfrac{1}{{0.00125}} + 54 = 800 + 54 = 854 ^oC = 854 + 273 = 1127K

The temperature when the resistance will be 2 Ohm is 1127 K. So, option (A) is correct.

Note: There may be a chance of making mistakes by simply dividing the resistance difference (1Ω1\Omega here) by the temperature coefficient (α\alpha ) and adding that to the existing temperature (300 K). But that can’t be done here because the R0{R_0} term is multiplied with α\alpha also (see eq.(1)). So be careful not to make this common mistake.