Two constant volume and two isentropic processes
Two constant pressure and two isentropic processes
Two constant volume and two isothermal processes
One constant pressure, one constant volume and two isentropic processes
A. Two constant volume and two isentropic processes
Ru × T
1.5 Ru × T
2 Ru × T
3 Ru × T
(m - 1)/ (2m - 1)
(2m - 1)/ (m - 1)
(m - 2)/ (3m - 4)
(m - 2)/ (5m - 4)
log (p1p2)/log (v1v2)
log (p2/ p1)/log (v1/ v2)
log (v1/ v2)/ log (p1/p2)
log [(p1v1)/(p2v2)]
Q1 - 2 = dU + W1 - 2
Q1 - 2 = dU - W1 - 2
Q1 - 2 = dU/W1 - 2
Q1 - 2 = dU × W1 - 2
Half
Same amount
Double
One-fourth
Fixed at both ends
Fixed at one end and free at the other end
Supported at its ends
Supported on more than two supports
Same
More
Less
Unpredictable
Cd⁴/D3n
Cd⁴/2D3n
Cd⁴/4D3n
Cd⁴/8D3n
Pressure and temperature
Temperature and volume
Heat and work
All of these
L = l/2
L = l/√2
L = l
L = 2l
Its length is very small
Its cross-sectional area is small
The ratio of its length to the least radius of gyration is less than 80
The ratio of its length to the least radius of gyration is more than 80
Equal to
Less than
Greater than
None of these
Th > Ts
Th < Ts
Th = Ts
None of these
Zero
Minimum
Maximum
Infinity
Homogeneous
Inelastic
Isotropic
Isentropic
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.
The indirect heat exchanger and cooler is avoided
Direct combustion system is used
A condenser is used
All of the above
Mass of oxygen in 1 kg of flue gas to the mass of oxygen in 1 kg of fuel
Mass of oxygen in 1 kg of fuel to the mass of oxygen in 1 kg of flue gas
Mass of carbon in 1 kg of flue gas to the mass of carbon in 1 kg of fuel
Mass of carbon in 1 kg of fuel to the mass of carbon in 1 kg of flue gas
Workdone
Entropy
Enthalpy
None of these
Boyle's law
Charles' law
Gay-Lussac law
Avogadro's law
23.97 bar
25 bar
26.03 bar
34.81 bar
(σx/2) + (1/2) × √(σx² + 4 τ²xy)
(σx/2) - (1/2) × √(σx² + 4 τ²xy)
(σx/2) + (1/2) × √(σx² - 4 τ²xy)
(1/2) × √(σx² + 4 τ²xy)
Longitudinal stress to longitudinal strain
Volumetric stress to volumetric strain
Lateral stress to Lateral strain
Shear stress to shear strain
πd²/4
πd²/16
πd3/16
πd3/32
Chain riveted joint
Diamond riveted joint
Crisscross riveted joint
Zigzag riveted joint
Gas engine
Petrol engine
Steam engine
Reversible engine
Increasing the highest temperature
Decreasing the highest temperature
Increasing the lowest temperature
Keeping the lowest temperature constant
Dual combustion cycle
Diesel cycle
Atkinson cycle
Rankine cycle
Carnot cycle
Rankine cycle
Brayton cycle
Bell Coleman cycle
Tensile strain increases more quickly
Tensile strain decreases more quickly
Tensile strain increases in proportion to the stress
Tensile strain decreases in proportion to the stress