Heat transfer is constant
Work transfer is constant
Mass flow at inlet and outlet is same
All of these
D. All of these
Zero
Minimum
Maximum
Positive
Drying and crushing the coal to a fine powder
Moulding the finely ground coal under pressure with or without a binding material
Heating the wood with a limited supply of air to temperature not less than 280°C
None of the above
Workdone
Entropy
Enthalpy
None of these
Carnot cycle
Bell-Coleman cycle
Rankine cycle
Stirling cycle
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.
cv/ cp =R
cp - cv = R
cv = R/ γ-1
Both (B) and (C)
Isothermal process
Hyperbolic process
Adiabatic process
Polytropic process
Zero
Minimum
Maximum
Infinity
23.97 bar
25 bar
26.03 bar
34.81 bar
Greater than
Less than
Equal to
None of these
(σx/2) + (1/2) × √(σx² + 4 τ²xy)
(σx/2) - (1/2) × √(σx² + 4 τ²xy)
(σx/2) + (1/2) × √(σx² - 4 τ²xy)
(1/2) × √(σx² + 4 τ²xy)
Carnot cycle
Rankine cycle
Brayton cycle
Bell Coleman cycle
Area at the time of fracture
Original cross-sectional area
Average of (A) and (B)
Minimum area after fracture
The first row
The second row
The central row
One rivet hole of the end row
Axis of load
Perpendicular to the axis of load
Maximum moment of inertia
Minimum moment of inertia
Sum of two principal stresses
Difference of two principal stresses
Half the sum of two principal stresses
Half the difference of two principal stresses
3/7
7/3
11/3
3/11
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
Middle of bar
Supported end
Bottom end
None of these
Th > Ts
Th < Ts
Th = Ts
None of these
Reversible cycles
Irreversible cycles
Semi-reversible cycles
Quasi-static cycles
300° to 500°C
500° to 700°C
700° to 900°C
900° to 1100°C
For a given compression ratio, both Otto and Diesel cycles have the same efficiency.
For a given compression ratio, Otto cycle is more efficient than Diesel cycle.
For a given compression ratio, Diesel cycle is more efficient than Otto cycle.
The efficiency of Otto or Diesel cycle has nothing to do with compression ratio.
-140 kJ
-80 kJ
-40 kJ
+60 kJ
Equal to
Less than
Greater than
None of these
Sum of two specific heats
Difference of two specific heats
Product of two specific heats
Ratio of two specific heats
Conservation of work
Conservation of heat
Conversion of heat into work
Conversion of work into heat
Temperature limits
Pressure ratio
Volume compression ratio
Cut-off ratio and compression ratio
Increases power output
Improves thermal efficiency
Reduces exhaust temperature
Do not damage turbine blades
Plastic limit
Elastic limit
Yield point
Limit of proportionality