Isothermal expansion
Isentropic expansion
Isothermal compression
Isentropic compression
C. Isothermal compression
Two constant volume and two isentropic processes
Two constant volume and two isothermal processes
Two constant pressure and two isothermal processes
One constant volume, one constant pressure and two isentropic processes
3 to 6
5 to 8
15 to 20
20 to 30
Fixed at both ends
Fixed at one end and free at the other end
Supported on more than two supports
Extending beyond the supports
WD3n/Cd⁴
2WD3n/Cd⁴
4WD3n/Cd⁴
8WD3n/Cd⁴
Reversible process
Irreversible process
Reversible or irreversible process
None of these
(p - 2d) t × σc
(p - d) t × τ
(p - d) t × σt
(2p - d) t × σt
23.97 bar
25 bar
26.03 bar
34.81 bar
3 to 6
5 to 8
10 to 20
15 to 30
Enthalpy
Internal energy
Entropy
External energy
The closed cycle gas turbine plants are external combustion plants.
In the closed cycle gas turbine, the pressure range depends upon the atmospheric pressure.
The advantage of efficient internal combustion is eliminated as the closed cycle has an external surface.
In open cycle gas turbine, atmosphere acts as a sink and no coolant is required.
Same
More
Less
Unpredictable
Young's modulus
Bulk modulus
Modulus of rigidity
Modulus of elasticity
Carnot cycle can't work with saturated steam
Heat is supplied to water at temperature below the maximum temperature of the cycle
A Rankine cycle receives heat at two places
Rankine cycle is hypothetical
65° to 220°C
220° to 345°C
345° to 470°C
470° to 550°C
2/3
3/4
1
9/8
Extensive heat is transferred
Extensive work is done
Extensive energy is utilised
None of these
d/4
d/8
d/12
d/16
3/7
7/3
11/3
3/11
1
1.4
1.45
2.3
Young's modulus
Modulus of rigidity
Bulk modulus
Poisson's ratio
Two constant pressure
Two constant volume
Two isentropic
One constant pressure, one constant volume
Proportional limit, elastic limit, yielding, failure
Elastic limit, proportional limit, yielding, failure
Yielding, proportional limit, elastic limit, failure
None of the above
Plasticity
Elasticity
Ductility
Malleability
No heat enters or leaves the gas
The temperature of the gas changes
The change in internal energy is equal to the mechanical workdone
All of the above
Increase
Decrease
Remain unchanged
Increase/decrease depending on application
Steel only
Concrete only
Steel and concrete both
None of these
Conservation of work
Conservation of heat
Conversion of heat into work
Conversion of work into heat
Change the shape of the beam
Effect the saving in material
Equalise the strength in tension and compression
Increase the cross-section of the beam
E = 3K.C/(3K + C)
E = 6K.C/(3K + C)
E = 9K.C/(3K + C)
E = 12K.C/(3K + C)
πd²/4
πd²/16
πd3/16
πd3/32