Greater than Carnot cycle
Less than Carnot cycle
Equal to Carnot cycle
None of these
B. Less than Carnot cycle
Zero
Minimum
Maximum
Infinity
Volumetric stress and volumetric strain
Lateral stress and lateral strain
Longitudinal stress and longitudinal strain
Shear stress to shear strain
It does not exist
It is more sensitive to changes in both metallurgical and mechanical conditions
It gives a more accurate picture of the ductility
It can be correlated with stress strain values in other tests like torsion, impact, combined stress tests etc.
(Net work output)/(Workdone by the turbine)
(Net work output)/(Heat supplied)
(Actual temperature drop)/(Isentropic temperature drop)
(Isentropic increase in temperature)/(Actual increase in temperature)
Yield point
Limit of proportionality
Breaking point
Elastic limit
Two isothermals and two isentropic
Two isentropic and two constant volumes
Two isentropic, one constant volume and one constant pressure
Two isentropic and two constant pressures
Decrease in cut-off
Increase in cut-off
Constant cut-off
None of these
3/7
7/3
11/3
3/11
mR (T2 - T1)
mcv (T2 - T1)
mcp (T2 - T1)
mcp (T2 + T1)
Cd⁴/D3n
Cd⁴/2D3n
Cd⁴/4D3n
Cd⁴/8D3n
Vapour
Perfect gas
Air
Steam
Thermal stresses
Tensile stress
Bending
No stress
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
Short column
Long column
Weak column
Medium column
Equal to
Less than
Greater than
None of these
Boyle's law
Charles' law
Gay-Lussac law
Joule's law
Always in single shear
Always in double shear
Either in single shear or double shear
None of these
3p/E × (2/m - 1)
3p/E × (2 - m)
3p/E × (1 - 2/m)
E/3p × (2/m - 1)
1
1.4
1.45
2.3
Isothermal process
Hyperbolic process
Adiabatic process
Polytropic process
It is impossible to construct an engine working on a cyclic process, whose sole purpose is to convert heat energy into work.
It is impossible to transfer heat from a body at a lower temperature to a higher temperature, without the aid of an external source.
There is a definite amount of mechanical energy, which can be obtained from a given quantity of heat energy.
All of the above
d/4
d/8
d/12
d/16
Thermodynamic law
Thermodynamic process
Thermodynamic cycle
None of these
Conservation of work
Conservation of heat
Conversion of heat into work
Conversion of work into heat
Equal to
Less than
Greater than
None of these
Greater than Carnot cycle
Less than Carnot cycle
Equal to Carnot cycle
None of these
Cracking
Carbonisation
Fractional distillation
Full distillation
pv = C
pv = m R T
pvn = C
pvγ = C
Strains
Stress and strain
Shear stress and shear strain
Moduli and elasticity
Breaking stress
Fracture stress
Yield point stress
Ultimate tensile stress