No heat enters or leaves the gas
The temperature of the gas changes
The change in internal energy is equal to the mechanical workdone
All of the above
D. All of the above
Isothermal process
Hyperbolic process
Adiabatic process
Polytropic process
In tension
In compression
Neither in tension nor in compression
None of these
The liquid fuels have higher calorific value than solid fuels
The solid fuels have higher calorific value than liquid fuels
A good fuel should have low ignition point
The liquid fuels consist of hydrocarbons
Tensile
Compressive
Shear
Zero
Steel only
Concrete only
Steel and concrete both
None of these
Thermal stresses
Tensile stress
Bending
No stress
Heat
Work
Internal energy
Entropy
1 kg of water
7 kg of water
8 kg of water
9 kg of water
Straight line
Parabolic
Elliptical
Cubic
Long
Medium
Short
None of these
Wood
Coke
Anthracite coal
Pulverised coal
(p - 2d) t × σc
(p - d) t × τ
(p - d) t × σt
(2p - d) t × σt
23.97 bar
25 bar
26.03 bar
34.81 bar
Otto cycle is more efficient than Diesel cycle
Diesel cycle is more efficient than Otto cycle
Dual cycle is more efficient than Otto and Diesel cycles
Dual cycle is less efficient than Otto and Diesel cycles
Oxygen
Sulphur
Nitrogen
Carbon
Elastic limit
Yield stress
Ultimate stress
Breaking stress
800 K
1000 K
1200 K
1400 K
Coke
Wood charcoal
Bituminous coal
Briquetted coal
65° to 220°C
220° to 345°C
345° to 470°C
470° to 550°C
Two constant volume and two isentropic processes
Two constant volume and two isothermal processes
Two constant pressure and two isothermal processes
One constant volume, one constant pressure and two isentropic processes
Q1 - 2 = dU + W1 - 2
Q1 - 2 = dU - W1 - 2
Q1 - 2 = dU/W1 - 2
Q1 - 2 = dU × W1 - 2
The failure of column occurs due to buckling alone
The length of column is very large as compared to its cross-sectional dimensions
The column material obeys Hooke's law
All of the above
Plasticity
Elasticity
Ductility
Malleability
3 to 6
5 to 8
10 to 20
15 to 30
65° to 220°C
220° to 345°C
345° to 470°C
470° to 550°C
Pressure and temperature
Temperature and volume
Heat and work
All of these
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.
1/8
1/4
1/2
2
Equal to
Less than
Greater than
None of these
Boyle's law
Charles' law
Gay-Lussac law
Avogadro's law