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Question: A metal bar of mass 1.5 kg is heated at atmospheric pressure. Its temperature has increased from \(3...

A metal bar of mass 1.5 kg is heated at atmospheric pressure. Its temperature has increased from 3030^\circ to 6060^\circ. Then the work done in the process is:
(Volume expansion coefficient=5×105C15\times {{10}^{-5}}{}^\circ {{C}^{-1}}
Density of metal=9×103kg/m39\times 10^3 kg/m^3
Atmospheric pressure= 10510^5 Pa)
A.25×103J B.2.5×103J C.12.5×103J D.1.25×103J \begin{aligned} & A.25\times {{10}^{-3}}J \\\ & B.2.5\times {{10}^{-3}}J \\\ & C.12.5\times {{10}^{-3}}J \\\ & D.1.25\times {{10}^{-3}}J \\\ \end{aligned}

Explanation

Solution

Hint: We have to know the thermodynamic formula for work done on a system. Also, we will use the mathematical expression for volume expansion coefficient. Then, simply using the given data, the answer can be found.

Formula used:
dW=pdVdW=p dV
β=1V.(δVδT)p\beta =\dfrac{1}{V}.{{\left( \dfrac{\delta V}{\delta T} \right)}_{p}}

Complete step-by-step solution:
Let, ρ=9×103kg/m3\rho =9\times {{10}^{3}}kg/{{m}^{3}}, which is the density of the metal. And m=1.5m=1.5 kg be its mass. The work done in a thermodynamic system is given by, dW=p.dVdW=p.dV. Here p is pressure and ‘dV’ is the change in volume. But the question only says about change in temperature but not in volume. So, we need to modify the formula.
Volume is a function of temperature and pressure. So,
V=V(p,T)V=V(p,T).
Taking differential, we obtain,
dV=(δVδT)p.dT+(δVδp)T.dpdV={{\left( \dfrac{\delta V}{\delta T} \right)}_{p}}.dT+{{\left( \dfrac{\delta V}{\delta p} \right)}_{T}}.dp
Here, (δVδT)p{{\left( \dfrac{\delta V}{\delta T} \right)}_{p}} is the rate of change of volume with temperature at constant pressure and (δVδp)T{{\left( \dfrac{\delta V}{\delta p} \right)}_{T}} is the rate of change of volume with pressure at a constant temperature. dT=(6030)=30dT=(60-30)=30 is the change in temperature.
In the given problem, pressure is constant. So, dp=0dp=0. Putting this in the above equation, we get
dV=(δVδT)p.dTdV={{\left( \dfrac{\delta V}{\delta T} \right)}_{p}}.dT
Now, volume expansion coefficient is given by β\beta .
β=1V.(δVδT)p\beta =\dfrac{1}{V}.{{\left( \dfrac{\delta V}{\delta T} \right)}_{p}}
(δVδT)p=β.V=β.mρ\Rightarrow \left(\dfrac{\delta V}{\delta T}\right)_p=\beta .V=\beta .\dfrac{m}{\rho}
Therefore,
dW=p.dV=p.(δVδT)p.dT=pβmρ.dT dW=105×5×105×1.59×103×30=25×103J \begin{aligned} & dW=p.dV=p.{{\left( \dfrac{\delta V}{\delta T} \right)}_{p}}.dT=p\beta \dfrac{m}{\rho }.dT \\\ & dW={{10}^{5}}\times 5\times {{10}^{-5}}\times \dfrac{1.5}{9\times {{10}^{3}}}\times 30=25\times {{10}^{-3}}J \\\ \end{aligned}
So, option A is the correct answer.

Additional information:
In physics, when work is done by a system, it is positive work. And when work is done against the system, it is negative work. However, in chemistry the opposite is believed.

Note: Remember the following things,
1. In this problem, dT only means the difference in temperature. Its value is the same for Kelvin and °C scale.
2. Don’t try to calculate work by first law of thermodynamics here. Because we don’t know the internal energy.
3. If the work is done in constant temperature, put dT=0dT=0 in the expression of ‘dV’ and make dp0dp \neq 0 and use corresponding given data.