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qUESTIONS

11th-jee

5.6 litre of helium gas at STP is adiabatically compressed to 0.7 litre. Taking the initial temperature to be T₁, the work done in the process is

11th-jee

A Carnot engine has an efficiency of 1/6. When the temperature of the sink is reduced by 62°C, its efficiency is doubled. The temperatures of the source and the sink are respectively

11th-jee

Which of the following is an equivalent cyclic process corresponding to the thermodynamic cyclic given in the figure? where, 1→2 is adiabatic. (Graphs are schematic and are not to scale)

11th-jee

A thermodynamic cycle xyzx is shown on a V-T diagram. The P-V diagram that best describes this cycle is:

11th-jee

Under an adiabatic process, the volume of an ideal gas gets doubled. Consequently the mean collision time between the gas molecules changes from τ₁ to τ₂. If Cp/ Cv= γ for this gas, then a good estimate for τ₁/τ₂ is given by

11th-jee

A litre of dry air at STP expands adiabatically to a volume of 3 litres. If γ= 1.40, the work done by air is: (3^1.4 = 4.6555) (Take air to be an ideal gas]

11th-jee

A cylinder with fixed capacity of 67.2 litre contains helium gas at STP: The amount of heat needed to raise the temperature of the gas by 20°C is [Given that R = 8.31 J mol^-¹K^-1]

11th-jee

In a given process for an ideal gas, dW = 0 and dQ<0 Then for the gas

11th-jee

A perfect gas goes from state A to another state B by absorbing 8×10^5 J of heat and doing 6.5×10^5 J of external work. It is now transferred between the same two states in another process in which it absorbs 10^5 J of heat. Then in the second process

11th-jee

A gas is enclosed in a cylinder with a movable frictionless piston. Its initial thermodynamic state at pressure Pi = 10^5 Pa and volume Vi = 10^-3 m3 changes to a final state at Pf = (1/32) × 10^5 Pa and Vf = 8 × 10^-3 m3 in an adiabatic quasi-static process, such that P3 V5 = constant. Consider another thermodynamic process that brings the system from the same initial state to the same final state in two steps: an isobaric expansion at Pi followed by an isochoric (isovolumetric) process at volume Vf. The amount of heat supplied to the system in the two-step process is approximately

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