Thermodynamic Processes
PHXI12:THERMODYNAMICS

371555 In a given process \(dW = 0,\,\,dQ < 0\) then for a gas

1 Temperature increases
2 Volume decreases
3 Pressure decreases
4 Pressure increases
PHXI12:THERMODYNAMICS

371556 If \(R = \) universal gas constant, the amount of heat needed to rise the temperature of \(2\;\,mol\) of an ideal monoatomic gas from \(273\;K\) to \(373\;K\) when no work is done is

1 \(100R\)
2 \(150R\)
3 \(300R\)
4 \(500R\)
PHXI12:THERMODYNAMICS

371557 In an isochoric process, the correct ratio is

1 \(\Delta Q: W=1: 1\)
2 \(\Delta Q: W=\gamma: \gamma-1\)
3 \(\Delta Q: W=\gamma-1: \gamma\)
4 \(\Delta Q: W=\gamma: 1\)
PHXI12:THERMODYNAMICS

371558 Figure shows the pressure versus temperature curves for a given mass of a gas corresponding to two different volumes \({V_{1}}\) and \({V_{2}}\), then:
supporting img

1 \({V_{1}>V_{2}}\)
2 \({V_{1} < V_{2}}\)
3 \({V_{1}=V_{2}}\)
4 The information is insufficient
PHXI12:THERMODYNAMICS

371559 \(0.08\;kg\) air is heated at constant volume through \(5^\circ \,C\). The specific heat of air at constant volume is\(0.17\,kcal{\rm{/}}kg^\circ \,C\) and\(J = 4.18\,\,joule{\rm{/}}cal\). The change in its internal energy is approximately.

1 \(298\;J\)
2 \(284\;J\)
3 \(318\;J\)
4 \(142\;J\)
PHXI12:THERMODYNAMICS

371555 In a given process \(dW = 0,\,\,dQ < 0\) then for a gas

1 Temperature increases
2 Volume decreases
3 Pressure decreases
4 Pressure increases
PHXI12:THERMODYNAMICS

371556 If \(R = \) universal gas constant, the amount of heat needed to rise the temperature of \(2\;\,mol\) of an ideal monoatomic gas from \(273\;K\) to \(373\;K\) when no work is done is

1 \(100R\)
2 \(150R\)
3 \(300R\)
4 \(500R\)
PHXI12:THERMODYNAMICS

371557 In an isochoric process, the correct ratio is

1 \(\Delta Q: W=1: 1\)
2 \(\Delta Q: W=\gamma: \gamma-1\)
3 \(\Delta Q: W=\gamma-1: \gamma\)
4 \(\Delta Q: W=\gamma: 1\)
PHXI12:THERMODYNAMICS

371558 Figure shows the pressure versus temperature curves for a given mass of a gas corresponding to two different volumes \({V_{1}}\) and \({V_{2}}\), then:
supporting img

1 \({V_{1}>V_{2}}\)
2 \({V_{1} < V_{2}}\)
3 \({V_{1}=V_{2}}\)
4 The information is insufficient
PHXI12:THERMODYNAMICS

371559 \(0.08\;kg\) air is heated at constant volume through \(5^\circ \,C\). The specific heat of air at constant volume is\(0.17\,kcal{\rm{/}}kg^\circ \,C\) and\(J = 4.18\,\,joule{\rm{/}}cal\). The change in its internal energy is approximately.

1 \(298\;J\)
2 \(284\;J\)
3 \(318\;J\)
4 \(142\;J\)
PHXI12:THERMODYNAMICS

371555 In a given process \(dW = 0,\,\,dQ < 0\) then for a gas

1 Temperature increases
2 Volume decreases
3 Pressure decreases
4 Pressure increases
PHXI12:THERMODYNAMICS

371556 If \(R = \) universal gas constant, the amount of heat needed to rise the temperature of \(2\;\,mol\) of an ideal monoatomic gas from \(273\;K\) to \(373\;K\) when no work is done is

1 \(100R\)
2 \(150R\)
3 \(300R\)
4 \(500R\)
PHXI12:THERMODYNAMICS

371557 In an isochoric process, the correct ratio is

1 \(\Delta Q: W=1: 1\)
2 \(\Delta Q: W=\gamma: \gamma-1\)
3 \(\Delta Q: W=\gamma-1: \gamma\)
4 \(\Delta Q: W=\gamma: 1\)
PHXI12:THERMODYNAMICS

371558 Figure shows the pressure versus temperature curves for a given mass of a gas corresponding to two different volumes \({V_{1}}\) and \({V_{2}}\), then:
supporting img

1 \({V_{1}>V_{2}}\)
2 \({V_{1} < V_{2}}\)
3 \({V_{1}=V_{2}}\)
4 The information is insufficient
PHXI12:THERMODYNAMICS

371559 \(0.08\;kg\) air is heated at constant volume through \(5^\circ \,C\). The specific heat of air at constant volume is\(0.17\,kcal{\rm{/}}kg^\circ \,C\) and\(J = 4.18\,\,joule{\rm{/}}cal\). The change in its internal energy is approximately.

1 \(298\;J\)
2 \(284\;J\)
3 \(318\;J\)
4 \(142\;J\)
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PHXI12:THERMODYNAMICS

371555 In a given process \(dW = 0,\,\,dQ < 0\) then for a gas

1 Temperature increases
2 Volume decreases
3 Pressure decreases
4 Pressure increases
PHXI12:THERMODYNAMICS

371556 If \(R = \) universal gas constant, the amount of heat needed to rise the temperature of \(2\;\,mol\) of an ideal monoatomic gas from \(273\;K\) to \(373\;K\) when no work is done is

1 \(100R\)
2 \(150R\)
3 \(300R\)
4 \(500R\)
PHXI12:THERMODYNAMICS

371557 In an isochoric process, the correct ratio is

1 \(\Delta Q: W=1: 1\)
2 \(\Delta Q: W=\gamma: \gamma-1\)
3 \(\Delta Q: W=\gamma-1: \gamma\)
4 \(\Delta Q: W=\gamma: 1\)
PHXI12:THERMODYNAMICS

371558 Figure shows the pressure versus temperature curves for a given mass of a gas corresponding to two different volumes \({V_{1}}\) and \({V_{2}}\), then:
supporting img

1 \({V_{1}>V_{2}}\)
2 \({V_{1} < V_{2}}\)
3 \({V_{1}=V_{2}}\)
4 The information is insufficient
PHXI12:THERMODYNAMICS

371559 \(0.08\;kg\) air is heated at constant volume through \(5^\circ \,C\). The specific heat of air at constant volume is\(0.17\,kcal{\rm{/}}kg^\circ \,C\) and\(J = 4.18\,\,joule{\rm{/}}cal\). The change in its internal energy is approximately.

1 \(298\;J\)
2 \(284\;J\)
3 \(318\;J\)
4 \(142\;J\)
PHXI12:THERMODYNAMICS

371555 In a given process \(dW = 0,\,\,dQ < 0\) then for a gas

1 Temperature increases
2 Volume decreases
3 Pressure decreases
4 Pressure increases
PHXI12:THERMODYNAMICS

371556 If \(R = \) universal gas constant, the amount of heat needed to rise the temperature of \(2\;\,mol\) of an ideal monoatomic gas from \(273\;K\) to \(373\;K\) when no work is done is

1 \(100R\)
2 \(150R\)
3 \(300R\)
4 \(500R\)
PHXI12:THERMODYNAMICS

371557 In an isochoric process, the correct ratio is

1 \(\Delta Q: W=1: 1\)
2 \(\Delta Q: W=\gamma: \gamma-1\)
3 \(\Delta Q: W=\gamma-1: \gamma\)
4 \(\Delta Q: W=\gamma: 1\)
PHXI12:THERMODYNAMICS

371558 Figure shows the pressure versus temperature curves for a given mass of a gas corresponding to two different volumes \({V_{1}}\) and \({V_{2}}\), then:
supporting img

1 \({V_{1}>V_{2}}\)
2 \({V_{1} < V_{2}}\)
3 \({V_{1}=V_{2}}\)
4 The information is insufficient
PHXI12:THERMODYNAMICS

371559 \(0.08\;kg\) air is heated at constant volume through \(5^\circ \,C\). The specific heat of air at constant volume is\(0.17\,kcal{\rm{/}}kg^\circ \,C\) and\(J = 4.18\,\,joule{\rm{/}}cal\). The change in its internal energy is approximately.

1 \(298\;J\)
2 \(284\;J\)
3 \(318\;J\)
4 \(142\;J\)