δQ = T.ds
δQ = T/ds
dQ = ds/T
None of these
A. δQ = T.ds
l/δl
δl/l
l.δl
l + δl
One-half
One-third
Two-third
Three-fourth
A Joule cycle consists of two constant volume and two isentropic processes.
An Otto cycle consists of two constant volume and two isentropic processes.
An Ericsson cycle consists of two constant pressure and two isothermal processes.
All of the above
Unit mass
Modulus of rigidity
Bulk modulus
Modulus of Elasticity
Carnot cycle can't work with saturated steam
Heat is supplied to water at temperature below the maximum temperature of the cycle
A Rankine cycle receives heat at two places
Rankine cycle is hypothetical
Area of cross-section of the column
Length and least radius of gyration of the column
Modulus of elasticity for the material of the column
All of the above
Elastic point of the material
Plastic point of the material
Breaking point of the material
Yielding point of the material
Ultimate shear stress of the column
Factor of safety
Torque resisting capacity
Slenderness ratio
1.333 N/m2
13.33 N/m2
133.3 N/m2
1333 N/m2
Reversible cycles
Irreversible cycles
Semi-reversible cycles
Quasi-static cycles
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
In the middle
At the tip below the load
At the support
Anywhere
Maximum at periphery and zero at center
Maximum at center
Uniform throughout
None of the above
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
Short column
Long column
Weak column
Medium column
8.314 J/kg mole-K
83.14 J/kgmole-K
831.4 J/kgmole-K
8314 J/kgmole-K
The liquid fuels consist of hydrocarbons.
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.
Its temperature increases but volume decreases
Its volume increases but temperature decreases
Both temperature and volume increases
Both temperature and volume decreases
4/7
11/4
9/7
All of these
kJ
kJ/kg
kJ/m2
kJ/m3
Tension
Compression
Bearing
Any one of the above
Absolute scale of temperature
Absolute zero temperature
Absolute temperature
None of these
Very low
Low
High
Very high
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
Increase
Decrease
Remain unchanged
Increase/decrease depending on application
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
2
4
8
16
Change in volume to original volume
Change in length to original length
Change in cross-sectional area to original cross-sectional area
Any one of the above
Cracking
Carbonisation
Fractional distillation
Full distillation
2ε₁ - ε₂
2ε₁ + ε₂
2ε₂ - ε₁
2ε₂ + ε₁