0°C
273°C
273 K
None of these
D. None of these
Double
Half
Same
None of these
Increases
Decreases
First increases and then decreases
First decreases and then increases
Reversible cycle
Irreversible cycle
Thermodynamic cycle
None of these
Homogeneous
Inelastic
Isotropic
Isentropic
Acts at a point on a beam
Spreads non-uniformly over the whole length of a beam
Spreads uniformly over the whole length of a beam
Varies uniformly over the whole length of a beam
Coal gas
Producer gas
Mond gas
Blast furnace gas
OC
OP
OQ
PQ
There is no change in temperature
There is no change in enthalpy
There is no change in internal energy
All of these
Increase in availability of energy
Increase in temperature
Decrease in pressure
Degradation of energy
Molecular mass of the gas and the gas constant
Atomic mass of the gas and the gas constant
Molecular mass of the gas and the specific heat at constant pressure
Molecular mass of the gas and the specific heat at constant volume
Increases the internal energy of the gas
Increases the temperature of the gas
Does some external work during expansion
Both (B) and (C)
Hookes law
Yield point
Plastic flow
Proof stress
Boyle's law
Charles' law
Gay-Lussac law
Avogadro's law
8.314 J/kg mole-K
83.14 J/kgmole-K
831.4 J/kgmole-K
8314 J/kgmole-K
Same
Twice
Four times
Eight times
Isothermal
Isentropic
Polytropic
None of these
Principal stress
Tensile stress
Compressive stress
Shear stress
The axis of load
An oblique plane
At right angles to the axis of specimen
Would not occur
In the middle
At the tip below the load
At the support
Anywhere
Zero
1/5
4/5
1
(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]
Mono-atomic
Di-atomic
Tri-atomic
Poly-atomic
Atomisation
Carbonisation
Combustion
None of these
Absolute scale of temperature
Absolute zero temperature
Absolute temperature
None of these
Its temperature increases but volume decreases
Its volume increases but temperature decreases
Both temperature and volume increases
Both temperature and volume decreases
Enthalpy
Internal energy
Entropy
External energy
Constant pressure cycle
Constant volume cycle
Constant temperature cycle
Constant temperature and pressure cycle
Pulverised coal
Brown coal
Coking bituminous coal
Non-coking bituminous coal
Total internal energy of a system during a process remains constant
Total energy of a system remains constant
Workdone by a system is equal to the heat transferred by the system
Internal energy, enthalpy and entropy during a process remain constant
All the reversible engines have the same efficiency.
All the reversible and irreversible engines have the same efficiency.
Irreversible engines have maximum efficiency.
All engines are designed as reversible in order to obtain maximum efficiency.