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JEE Advanced 2019Paper 1
Exam
JEE Advanced
Year
2019
Paper
Paper 1
Subject
Physics
Chapter
Thermal Properties of Matter

JEE Advanced 2019 · Paper 1 · Physics · Thermal Properties of Matter

A current carrying wire heats a metal rod. The wire provides a...

A current carrying wire heats a metal rod. The wire provides a constant power (P)\left(P\right) to the rod. The metal rod is enclosed in an insulated container. It is observed that the temperature (T)\left(T\right) in the metal rod changes with time \left(t\right)as:<br/>as:<br />T\left(t\right)=T0(1+βt1/4)= {T}_{0}\left(1 + \beta{t}^{1 / 4}\right)
where β\beta is a constant with appropriate dimension while ${T}_{0} is a constant with dimension of temperature. The heat capacity of the metal is:

Options

  1. A4P(T(t)−T0)β4T02\dfrac{4P\left(T\left(t\right) - {T}_{0}\right)}{{\beta}^{4}{T}_{0}^{2}}
  2. B4P(T(t)−T0)2β4T03\dfrac{4P{\left(T\left(t\right) - {T}_{0}\right)}^{2}}{{\beta}^{4}{T}_{0}^{3}}
  3. C4P(T(t)−T0)4β4T05\dfrac{4P{\left(T\left(t\right) - {T}_{0}\right)}^{4}}{{\beta}^{4}{T}_{0}^{5}}
  4. D4P(T(t)−T0)3β4T04\dfrac{4P{\left(T\left(t\right) - {T}_{0}\right)}^{3}}{{\beta}^{4}{T}_{0}^{4}}

Correct answer

D. 4P(T(t)−T0)3β4T04\dfrac{4P{\left(T\left(t\right) - {T}_{0}\right)}^{3}}{{\beta}^{4}{T}_{0}^{4}}

Step-by-step solution

Heat required for small increment in temperature of a substance is given by
dQ=m.s.dTdQ = m . s . dT
where, m=m = mass of substances
or s=s = specific heat of substance
Now, heat capacity, H=m.s.H = m . s .
∴dQ=H.dT∴ dQ = H . dT
⇒⇒ Rate of heat absorption by the rod, dQdt=P=H⋅dTdt\dfrac{dQ}{dt} = P = H ⋅ \dfrac{dT}{dt} .......(1)
But given that, temperature of rod as a function of time is
T=T0(1+βt1/4)T = {T}_{0}\left(1 + \beta{t}^{1 / 4}\right) ......(2)
⇒dTdt=T0⋅β⋅14t−34⇒ \dfrac{dT}{dt} = {T}_{0} ⋅ \beta ⋅ \dfrac{1}{4}{t}^{- \dfrac{3}{4}}
Putting it in (1) gives
P=H⋅T0⋅β⋅14⋅t−34P = H ⋅ {T}_{0} ⋅ \beta ⋅ \dfrac{1}{4} ⋅ {t}^{- \dfrac{3}{4}}
⇒H=4P⋅t3/4T0⋅β⇒ H = \dfrac{4P ⋅ {t}^{3 / 4}}{{T}_{0} ⋅ \beta}
⇒H=4P(T−T0)3T04⋅B4⇒ H = 4P\dfrac{{\left(T - {T}_{0}\right)}^{3}}{{T}_{0}^{4} ⋅ {B}^{4}}
Now using equation (2)( 2 )
T−T0=T0β⋅t1/4T - {T}_{0} = {T}_{0}\beta ⋅ {t}^{1 / 4}
⇒t3/4=T0(T−T0T0β)3⇒ {t}^{3 / 4} = {T}_{0}{\left(\dfrac{T - {T}_{0}}{{T}_{0}\beta}\right)}^{3}
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