Carnot
Ericsson
Stirling
None of the above
D. None of the above
Bearing stresses
Fatigue stresses
Crushing stresses
Resultant stresses
Constant pressure process
Constant volume process
Constant pvn process
All of these
11/7
9/7
4/7
All of the above
Zero
Minimum
Maximum
Positive
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
30 MN/m²
50 MN/m²
100 MN/m²
200 MN/m²
E = 3K.C/(3K + C)
E = 6K.C/(3K + C)
E = 9K.C/(3K + C)
E = 12K.C/(3K + C)
Reversible cycles
Irreversible cycles
Semi-reversible cycles
Adiabatic irreversible cycles
Ru × T
1.5 Ru × T
2 Ru × T
3 Ru × T
L = l/2
L = l/√2
L = l
L = 2l
Combustion is at constant volume
Expansion and compression are isentropic
Maximum temperature is higher
Heat rejection is lower
T.ω watts
2π. T.ω watts
2π. T.ω/75 watts
2π. T.ω/4500 watts
Oxygen
Sulphur
Nitrogen
Carbon
Tensile
Compressive
Shear
Zero
No stress
Shear stress
Tensile stress
Compressive stress
5WL³/ 384EI
WL³/384EI
WL³/ 348EI
WL³/ 48EI
Extensive heat is transferred
Extensive work is done
Extensive energy is utilised
None of these
(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)
Measure shear strain
Measure linear strain
Measure volumetric strain
Relieve strain
Increases power output
Improves thermal efficiency
Reduces exhaust temperature
Do not damage turbine blades
Plastic limit
Elastic limit
Yield point
Limit of proportionality
Doubled
Halved
Becomes four times
None of the above
External energy
Internal energy
Kinetic energy
Molecular energy
(11/3) CO2 + (3/7) CO
(3/7) CO2 + (11/3) CO
(7/3) CO2 + (3/11) CO
(3/11) CO2 + (7/3) CO
Principal stress
Tensile stress
Compressive stress
Shear stress
Yield point stress
Breaking stress
Ultimate stress
Elastic limit
8.314 J/kg mole-K
83.14 J/kgmole-K
831.4 J/kgmole-K
8314 J/kgmole-K
12
14
16
32
Long
Medium
Short
None of these
1 N-m/s
100 N-m
1000 N-m/s
1 × 106 N-m/s