Chapter 12: Problem 2
For an adiabatic expansion process, the quantity \(P V\) (A) decreases. (B) increases. (C) remains constant. (D) depends on adiabatic exponent of the gas.
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Chapter 12: Problem 2
For an adiabatic expansion process, the quantity \(P V\) (A) decreases. (B) increases. (C) remains constant. (D) depends on adiabatic exponent of the gas.
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Temperature of \(100 \mathrm{gm}\) water in changed from \(0^{\circ} \mathrm{C}\) to \(3^{\circ} \mathrm{C}\). In this process, heat supplied to water will be (specified heat of water \(=1 \mathrm{cal} / \mathrm{gm}{ }^{\circ} \mathrm{C}\) ) (A) Equal to \(300 \mathrm{cal}\) (B) Greater than \(300 \mathrm{cal}\) (C) Less than \(300 \mathrm{cal}\) (D) Data is insufficient
Three copper blocks of masses \(M_{1}, M_{2}\), and \(M_{3} \mathrm{~kg}\), respectively, are brought in to thermal contact till they reach equilibrium. Before contact, they were at \(T_{1}, T_{2}, T_{3}\left(T_{1}>T_{2}>T_{3}\right)\). Assuming there is no heat loss to the surroundings, the equilibrium temperature \(T\) is \((s\) is specific heat of copper) (A) \(T=\frac{T_{1}+T_{2}+T_{3}}{3}\) (B) \(T=\frac{M_{1} T_{1}+M_{2} T_{2}+M_{3} T_{3}}{M_{1}+M_{2}+M_{3}}\) (C) \(T=\frac{M_{1} T_{1}+M_{2} T_{2}+M_{3} T_{3}}{3\left(M_{1}+M_{2}+M_{3}\right)}\) (D) \(T=\frac{M_{1} T_{1} s+M_{2} T_{2} s+M_{3} T_{3} s}{M_{1}+M_{2}+M_{3}}\)
Water flows at the rate of \(0.1500 \mathrm{~kg} / \mathrm{min}\) through a tube and is heated by a heater dissipating \(25.2 \mathrm{~W}\). The inflow and outflow water temperatures are \(15.2^{\circ} \mathrm{C}\) and \(17.4^{\circ} \mathrm{C}\), respectively. When the rate of flow is increased to \(0.2318 \mathrm{~kg} / \mathrm{min}\) and the rate of heating to \(37.8 \mathrm{~W}\), the inflow and outflow temperatures are unaltered. Find: (A) The specific heat capacity of water. (B) The rate of loss of heat from the tube.
A vertical cylinder with a massless piston is filled with one mole of an ideal gas. The piston can move freely without friction. The piston is slowly raised so that the gas expands isothermally at temperature \(300 \mathrm{~K}\). The amount of work done in increasing the volume two times is \(R=\frac{25}{3} \mathrm{~J} / \mathrm{mol} / \mathrm{K}, \log _{\mathrm{e}} 2=0.7\) (A) \(1750 \mathrm{~J}\) (B) \(2500 \mathrm{~J}\) (C) \(750 \mathrm{~J}\) (D) \(4250 \mathrm{~J}\)
When a system is taken from state \(i\) to state \(f\) along the path iaf, it is found \(Q=50 \mathrm{cal}\) and \(W=20\) cal. Along the path \(i b f, Q=36\) cal. \(W\) along the path \(i b f\) is [2007] (A) \(6 \mathrm{cal}\) (B) \(16 \mathrm{cal}\) (C) \(66 \mathrm{cal}\) (D) \(14 \mathrm{cal}\)
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