Combustion is at constant volume
Expansion and compression are isentropic
Maximum temperature is higher
Heat rejection is lower
D. Heat rejection is lower
Reversible cycles
Irreversible cycles
Semi-reversible cycles
Quasi-static cycles
Wood
Coke
Anthracite coal
Pulverised coal
Pressure
Volume
Temperature
All of these
Dual combustion cycle
Diesel cycle
Atkinson cycle
Rankine cycle
Short columns
Long columns
Weak columns
Medium columns
Elements
Compounds
Atoms
Molecules
Brown coal
Peat
Coking bituminous coal
Non-coking bituminous coal
Zeroth
First
Second
Third
3/7
7/3
11/3
3/11
Perfect gas
Air
Steam
Ordinary gas
Th > Ts
Th < Ts
Th = Ts
None of these
Maximum shear stress
No shear stress
Minimum shear stress
None of the above
Workdone
Entropy
Enthalpy
None of these
When coal is first dried and then crushed to a fine powder by pulverising machine
From the finely ground coal by moulding under pressure with or without a binding material
When coal is strongly heated continuously for 42 to 48 hours in the absence of air in a closed vessel
By heating wood with a limited supply of air to a temperature not less than 280°C
Volume
Temperature
Mass
Energy
Of same magnitude as that of bar and applied at the lower end
Half the weight of bar applied at lower end
Half of the square of weight of bar applied at lower end
One fourth of weight of bar applied at lower end
Temperature limits
Pressure ratio
Compression ratio
Cut-off ratio and compression ratio
It is possible to transfer heat from a body at a lower temperature to a body at a higher temperature.
It is impossible to transfer heat from a body at a lower temperature to a body at a higher temperature, without the aid of an external source.
It is possible to transfer heat from a body at a lower temperature to a body at a higher temperature by using refrigeration cycle.
None of the above
Isothermal process
Hyperbolic process
Adiabatic process
Polytropic process
Equal to
Half
Double
Quadruple
Maximum cycle temperature
Minimum cycle temperature
Pressure ratio
All of these
4/7
11/4
9/7
All of these
Rankine
Stirling
Carnot
Brayton
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
0.5 s.l.σt
s.l.σt
√2 s.l.σt
2.s.l.σt
Zero
wl/4
wl/2
wl²/2
More
Less
Same
More/less depending on composition
Boyle's law
Charles' law
Gay-Lussac law
Avogadro's law
2.1 × 10⁵ kg/cm²
2.1 × 10⁶ kg/cm²
2.1 × 10⁷ kg/cm²
0.1 × 10⁶ kg/cm²
Increase
Decrease
Remain unchanged
Increase/decrease depending on application