Tensile in both the material
Tensile in steel and compressive in copper
Compressive in steel and tensile in copper
Compressive in both the materials
D. Compressive in both the materials
Increasing the highest temperature
Decreasing the highest temperature
Increasing the lowest temperature
Keeping the lowest temperature constant
Boyle's law
Charles' law
Gay-Lussac law
Avogadro's law
Law of equipartition of energy
Law of conservation of energy
Law of degradation of energy
None of these
Hookes law
Yield point
Plastic flow
Proof stress
Young's modulus
Bulk modulus
Modulus of rigidity
Poisson's ratio
Sum of two principal stresses
Difference of two principal stresses
Half the sum of two principal stresses
Half the difference of two principal stresses
Temperature limits
Pressure ratio
Volume compression ratio
Cut-off ratio and compression ratio
Maximum torque it can transmit
Number of cycles it undergoes before failure
Elastic limit up to which it resists torsion, shear and bending stresses
Torque required to produce a twist of one radian per unit length of shaft
Increases the internal energy of the gas
Increases the temperature of the gas
Does some external work during expansion
Both (B) and (C)
Double
Half
Same
None of these
Positive
Negative
Positive or negative
None of these
δQ = T.ds
δQ = T/ds
dQ = ds/T
None of these
δl = 4PE/ πl²
δl = 4πld²/PE
δl = 4Pl/πEd₁d₂
δl = 4PlE/ πd₁d₂
kJ
kJ/kg
kJ/m2
kJ/m3
Petrol engine
Diesel engine
Reversible engine
Irreversible engine
It is used as the alternate standard of comparison of all heat engines.
All the heat engines are based on Carnot cycle.
It provides concept of maximising work output between the two temperature limits.
All of the above
Isothermal expansion
Isentropic expansion
Isothermal compression
Isentropic compression
Proportional limit, elastic limit, yielding, failure
Elastic limit, proportional limit, yielding, failure
Yielding, proportional limit, elastic limit, failure
None of the above
0.287 J/kgK
2.87 J/kgK
28.7 J/kgK
287 J/kgK
wl/6
wl/3
wl
2wl/3
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
Specific heat at constant volume
Specific heat at constant pressure
kilo-Joule
None of these
The pressure and temperature of the working substance must not differ, appreciably, from those of the surroundings at any stage in the process
All the processes, taking place in the cycle of operation, must be extremely slow
The working parts of the engine must be friction free
All of the above
OC
OP
OQ
PQ
400 MPa
500 MPa
900 MPa
1400 MPa
Increase
Decrease
Remain unchanged
Increase/decrease depending on application
One
Two
Three
Four
pv = C
pv = m R T
pvn = C
pvγ = C
Carnot
Ericsson
Stirling
None of the above
Middle of bar
Supported end
Bottom end
None of these