Kh > Ks
Kh < Ks
Kh = Ks
None of these
A. Kh > Ks
kJ
kJ/kg
kJ/m2
kJ/m3
1
1.4
1.67
1.87
Maximum calculated value
Minimum calculated value
Mean value
Extreme value
12
14
16
32
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
Remains constant
Increases
Decreases
None of these
Its temperature will increase
Its volume will increase
Both temperature and volume will increase
Neither temperature not volume will increase
50 %
25 %
0 %
15 %
65° to 220°C
220° to 345°C
345° to 470°C
470° to 550°C
Boyle's law
Charles' law
Gay-Lussac law
Avogadro's law
Brayton cycle
Joule cycle
Carnot cycle
Reversed Brayton cycle
Increasing the highest temperature
Decreasing the highest temperature
Increasing the lowest temperature
Keeping the lowest temperature constant
Longitudinal stress to longitudinal strain
Volumetric stress to volumetric strain
Lateral stress to Lateral strain
Shear stress to shear strain
Sum of two specific heats
Difference of two specific heats
Product of two specific heats
Ratio of two specific heats
Strain energy
Resilience
Proof resilience
Modulus of resilience
Shear force changes sign
Shear force is maximum
Bending moment changes sign
Bending moment is maximum
Boyle
Charles
Joule
None of these
Same
Double
Half
One-fourth
Otto cycle
Ericsson cycle
Joule cycle
Stirling cycle
L = l/2
L = l/√2
L = l
L = 2l
Short columns
Long columns
Both short and long columns
Weak columns
Young's modulus
Bulk modulus
Modulus of rigidity
Modulus of elasticity
Always in single shear
Always in double shear
Either in single shear or double shear
None of these
Reversible cycles
Irreversible cycles
Semi-reversible cycles
Adiabatic irreversible cycles
Doubled
Halved
Becomes four times
None of the above
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
400 MPa
500 MPa
900 MPa
1400 MPa
Increasing the internal energy of gas
Doing some external work
Increasing the internal energy of gas and also for doing some external work
None of the above
0.086
1.086
1.086
4.086