Longitudinal stress to longitudinal strain
Volumetric stress to volumetric strain
Lateral stress to Lateral strain
Shear stress to shear strain
D. Shear stress to shear strain
Increase in availability of energy
Increase in temperature
Decrease in pressure
Degradation of energy
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
l/8
l/4
l/2
l
Thermal stresses
Tensile stress
Bending
No stress
Boyle's law
Charles' law
Gay-Lussac law
Avogadro's law
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
1
1.4
1.45
2.3
Principal stresses
Normal stresses on planes at 45°
Shear stresses on planes at 45°
Normal and shear stresses on a plane
K₁ K₂
(K₁ + K₂)/ 2
(K₁ + K₂)/ K₁ K₂
K₁ K₂/ (K₁ + K₂)
Same
Twice
Four times
Eight times
Carnot cycle
Rankine cycle
Brayton cycle
Bell Coleman cycle
Considerably greater than that necessary to continue it
Considerably lesser than that necessary to continue it
Greater than that necessary to stop it
Lesser than that necessary to stop it
Increase
Decrease
Remain unchanged
Increase/decrease depending on application
Short column
Long column
Weak column
Medium column
Carnot cycle
Stirling cycle
Otto cycle
None of these
Increases power output
Improves thermal efficiency
Reduces exhaust temperature
Do not damage turbine blades
Pressure
Volume
Temperature
Density
(σx + σy)/2 + (1/2) × √[(σx - σy)² + 4 τ²xy]
(σx + σy)/2 - (1/2) × √[(σx - σy)² + 4 τ²xy]
(σx - σy)/2 + (1/2) × √[(σx + σy)² + 4 τ²xy]
(σx - σy)/2 - (1/2) × √[(σx + σy)² + 4 τ²xy]
237°C
-273°C
-237°C
273°C
wl²/3√3
wl²/6√3
wl²/9√3
wl²/12√3
Maximum cycle temperature
Minimum cycle temperature
Pressure ratio
All of these
Zero
wl/4
wl/2
wl²/2
Calorific value
Heat energy
Lower calorific value
Higher calorific value
Th > Ts
Th < Ts
Th = Ts
None of these
Zeroth law of thermodynamics
First law of thermodynamics
Second law of thermodynamics
Kinetic theory of gases
Constant volume process
Adiabatic process
Constant pressure process
Isothermal process
Principal stress
Tensile stress
Compressive stress
Shear stress
Heat
Work
Internal energy
Entropy
Proportional limit, elastic limit, yielding, failure
Elastic limit, proportional limit, yielding, failure
Yielding, proportional limit, elastic limit, failure
None of the above
Area at the time of fracture
Original cross-sectional area
Average of (A) and (B)
Minimum area after fracture