Smaller end
Larger end
Middle
Anywhere
A. Smaller end
1 N-m/s
100 N-m
1000 N-m/s
1 × 106 N-m/s
wl²/3√3
wl²/6√3
wl²/9√3
wl²/12√3
rγ - 1
1 - rγ - 1
1 - (1/r) γ/γ - 1
1 - (1/r) γ - 1/ γ
Equal to
More than
Less than
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
Gas engine
Petrol engine
Steam engine
Reversible engine
Butt joint
Lap joint
Double riveted lap joints
All types of joints
log (p1p2)/log (v1v2)
log (p2/ p1)/log (v1/ v2)
log (v1/ v2)/ log (p1/p2)
log [(p1v1)/(p2v2)]
Absolute scale of temperature
Absolute zero temperature
Absolute temperature
None of these
Homogeneous
Inelastic
Isotropic
Isentropic
Same as
Less than
Greater than
None of these
Mono-atomic
Di-atomic
Tri-atomic
Poly-atomic
Same
Double
Half
Four times
Constant volume process
Adiabatic process
Constant pressure process
Isothermal process
M/I = σ/y = E/R
T/J = τ/R = Cθ/l
M/R = T/J = Cθ/l
T/l= τ/J = R/Cθ
(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)
Strain energy
Resilience
Proof resilience
Modulus of resilience
Area at the time of fracture
Original cross-sectional area
Average of (A) and (B)
Minimum area after fracture
Sum of two principal stresses
Difference of two principal stresses
Half the sum of two principal stresses
Half the difference of two principal stresses
Soft coal
Hard coal
Pulverised coal
Bituminous coal
Maximum shear stress
No shear stress
Minimum shear stress
None of the above
Fixed at both ends
Fixed at one end and free at the other end
Supported on more than two supports
Extending beyond the supports
WD3n/Cd⁴
2WD3n/Cd⁴
4WD3n/Cd⁴
8WD3n/Cd⁴
W1 - 2 = 0
Q1 - 2 = 0
dU = 0
All of these
Volume
Temperature
Mass
Energy
Zeroth
First
Second
Third
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
Short column
Long column
Weak column
Medium column
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
Short columns
Long columns
Both short and long columns
Weak columns