Tensile
Compressive
Shear
Zero
B. Compressive
Volumetric stress and volumetric strain
Lateral stress and lateral strain
Longitudinal stress and longitudinal strain
Shear stress to shear strain
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
Pulverised coal
Brown coal
Coking bituminous coal
Non-coking bituminous coal
Constant volume process
Adiabatic process
Constant pressure process
Isothermal process
pv = mRT
pv = RTm
pvm = C
pv = (RT)m
Smaller end
Larger end
Middle
Anywhere
3 to 6
5 to 8
15 to 20
20 to 30
Wl3 / 48EI
5Wl3 / 384EI
Wl3 / 392EI
Wl3 / 384EI
Cut-off is increased
Cut-off is decreased
Cut-off is zero
Cut-off is constant
Absolute pressure = Gauge pressure + Atmospheric pressure
Gauge pressure = Absolute pressure + Atmospheric pressure
Atmospheric pressure = Absolute pressure + Gauge pressure
Absolute pressure = Gauge pressure - Atmospheric pressure
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
Longitudinal stress to longitudinal strain
Volumetric stress to volumetric strain
Lateral stress to Lateral strain
Shear stress to shear strain
9/7
11/7
7/4
1/4
The material A is more ductile than material B
The material B is more ductile than material A
The ductility of material A and B is equal
The material A is brittle and material B is ductile
Young's modulus
Modulus of rigidity
Bulk modulus
Poisson's ratio
(σx + σy)/2 + (1/2) × √[(σx - σy)² + 4 τ²xy]
(σx + σy)/2 - (1/2) × √[(σx - σy)² + 4 τ²xy]
(σx - σy)/2 + (1/2) × √[(σx + σy)² + 4 τ²xy]
(σx - σy)/2 - (1/2) × √[(σx + σy)² + 4 τ²xy]
Elastic limit
Yield stress
Ultimate stress
Breaking stress
Enthalpy
Internal energy
Entropy
External energy
23.97 bar
25 bar
26.03 bar
34.81 bar
4 tonnes/ cm²
8 tonnes/ cm²
16 tonnes/ cm²
22 tonnes/ cm²
Petrol
Kerosene
Fuel oil
Lubricating oil
Carnot cycle
Stirling cycle
Otto cycle
Diesel cycle
Greater than
Less than
Equal to
None of these
Carnot cycle
Otto cycle
Joule's cycle
Stirling cycle
Boyle's law
Charles' law
Gay-Lussac law
All of these
rγ - 1
1 - rγ - 1
1 - (1/r) γ/γ - 1
1 - (1/r) γ - 1/ γ
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
Its length is very small
Its cross-sectional area is small
The ratio of its length to the least radius of gyration is less than 80
The ratio of its length to the least radius of gyration is more than 80
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
More
Less
Same
More/less depending on composition