A Carnot engine operates between 227°C and 27°C . Efficiency of the engine will be -
(1)
(2)
(3)
(4)
Efficiency of a Carnot engine is 50% when temperature of outlet is 500 K. In order to increase efficiency up to 60% keeping temperature of intake the same what is temperature of outlet ?
(1) 200 K
(2) 400 K
(3) 600 K
(4) 800 K
An ideal heat engine working between temperature T1 and T2 has an efficiency η, the new efficiency if both the source and sink temperature are doubled, will be
(1)
(2) η
(3) 2η
(4) 3η
An engine is supposed to operate between two reservoirs at temperature 727°C and 227°C. The maximum possible efficiency of such an engine is -
(1) 1/2
(2) 1/4
(3) 3/4
(4) 1
An ideal gas heat engine operates in Carnot cycle between 227°C and 127°C. It absorbs 6 × 104 cal of heat at higher temperature. Amount of heat converted to work is -
(1) 2.4 × 104 cal
(2) 6 × 104 cal
(3) 1.2 × 104 cal
(4) 4.8 × 104 cal
Which of the following processes is reversible ?
(1) Transfer of heat by radiation
(2) Electrical heating of a nichrome wire
(3) Transfer of heat by conduction
(4) Isothermal compression
A monoatomic ideal gas, initially at temperature T1, is enclosed in a cylinder fitted with a frictionless piston. The gas is allowed to expand adiabatically to a temperature T2 by releasing the piston suddenly. If L1 and L2 are the lengths of the gas column before and after expansion respectively, then T1/ T2 is given by -
(1)
(2)
(3)
(4)
A closed hollow insulated cylinder is filled with gas at \(0^{\circ}\mathrm{C}\) and also contains an insulated piston of negligible weight and negligible thickness at the middle point. The gas on one side of the piston is heated to \(100^{\circ}\mathrm{C}\).
If the piston moves 5 cm, the length of the hollow cylinder will be:
1. 13.65 cm
2. 27.3 cm
3. 38.6 cm
4. 64.6 cm
A monoatomic gas is supplied with the heat \(Q\) very slowly, keeping the pressure constant. The work done by the gas will be:
1. \({2 \over 3}Q\)
2. \({3 \over 5}Q\)
3. \({2 \over 5}Q\)
4. \({1 \over 5}Q\)
An ideal gas expands isothermally from a volume \(V_1\) to \(V_2\) and then is compressed to the original volume \(V_1\) adiabatically. The initial pressure is \(P_1\) and the final pressure is \(P_3.\) The total work done is \(W.\) Then:
1. \(𝑃 _3 > 𝑃 _1 , 𝑊 > 0\)
2. \(𝑃 _3 < 𝑃 _1 , 𝑊 < 0\)
3. \(𝑃 _3 > 𝑃 _1 , 𝑊 < 0\)
4. \(𝑃 _3 = 𝑃 _1 , 𝑊 = 0\)