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
B. All the heat engines are based on Carnot cycle.
Isothermal process
Hyperbolic process
Adiabatic process
Polytropic process
Two constant pressure
Two constant volume
Two isentropic
One constant pressure, one constant volume
Boyle's law
Charles' law
Gay-Lussac law
Joule's law
30 MN/m²
50 MN/m²
100 MN/m²
200 MN/m²
300° to 500°C
500° to 700°C
700° to 900°C
900° to 1100°C
Zero
wl/4
wl/2
wl²/2
Tensile
Compressive
Shear
Zero
Mass of oxygen in 1 kg of flue gas to the mass of oxygen in 1 kg of fuel
Mass of oxygen in 1 kg of fuel to the mass of oxygen in 1 kg of flue gas
Mass of carbon in 1 kg of flue gas to the mass of carbon in 1 kg of fuel
Mass of carbon in 1 kg of fuel to the mass of carbon in 1 kg of flue gas
Equal to
One-half
Twice
Four times
Peat
Lignite
Bituminous coal
Anthracite coal
The increase in entropy is obtained from a given quantity of heat at a low temperature.
The change in entropy may be regarded as a measure of the rate of the availability or unavailability of heat for transformation into work.
The entropy represents the maximum amount of work obtainable per degree drop in temperature.
All of the above
Coal gas
Producer gas
Mond gas
Blast furnace gas
pv = C
pv = m R T
pvn = C
pvγ = C
Yield point stress
Breaking stress
Ultimate stress
Elastic limit
50 %
25 %
20 %
30 %
It is possible to transfer heat from a body at a lower temperature to a body at a higher temperature.
It is impossible to transfer heat from a body at a lower temperature to a body at a higher temperature, without the aid of an external source.
It is possible to transfer heat from a body at a lower temperature to a body at a higher temperature by using refrigeration cycle.
None of the above
Toughness
Tensile strength
Capability of being cold worked
Hardness
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.
Partial combustion of coal, coke, anthracite coal or charcoal in a mixed air steam blast
Carbonisation of bituminous coal
Passing steam over incandescent coke
Passing air and a large amount of steam over waste coal at about 650°C
Isothermal process
Hyperbolic process
Adiabatic process
Polytropic process
Axis of load
Perpendicular to the axis of load
Maximum moment of inertia
Minimum moment of inertia
Proportional limit, elastic limit, yielding, failure
Elastic limit, proportional limit, yielding, failure
Yielding, proportional limit, elastic limit, failure
None of the above
Permanent
Temporary
Semi-permanent
None of these
Mild steel
Cast iron
Concrete
Bone of these
It is impossible to construct an engine working on a cyclic process, whose sole purpose is to convert heat energy into work
It is possible to construct an engine working on a cyclic process, whose sole purpose is to convert heat energy into work
It is impossible to construct a device which operates in a cyclic process and produces no effect other than the transfer of heat from a cold body to a hot body
None of the above
Homogeneous
Inelastic
Isotropic
Isentropic
Hookes law
Yield point
Plastic flow
Proof stress
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
Greater than Carnot cycle
Less than Carnot cycle
Equal to Carnot cycle
None of these
More
Less
Same
More/less depending on composition