Increases
Decreases
First increases and then decreases
First decreases and then increases
A. Increases
Sum of two principal stresses
Difference of two principal stresses
Half the sum of two principal stresses
Half the difference of two principal stresses
Top layer
Bottom layer
Neutral axis
Every cross-section
p.v = constant, if T is kept constant
v/T = constant, if p is kept constant
p/T = constant, if v is kept constant
T/p = constant, if v is kept constant
Wood charcoal
Bituminous coal
Briquetted coal
None of these
When coal is first dried and then crushed to a fine powder by pulverising machine
From the finely ground coal by moulding under pressure with or without a binding material
When coal is strongly heated continuously for 42 to 48 hours in the absence of air in a closed vessel
By heating wood with a limited supply of air to a temperature not less than 280°C
Cracking
Carbonisation
Fractional distillation
Full distillation
Tensile strain increases more quickly
Tensile strain decreases more quickly
Tensile strain increases in proportion to the stress
Tensile strain decreases in proportion to the stress
Load/original cross-sectional area and change in length/original length
Load/ instantaneous cross-sectional area and loge (original area/ instantaneous area)
Load/ instantaneous cross-sectional area and change in length/ original length
Load/ instantaneous area and instantaneous area/original area
Heat and work crosses the boundary of the system, but the mass of the working substance does not crosses the boundary of the system
Mass of the working substance crosses the boundary of the system but the heat and work does not crosses the boundary of the system
Both the heat and work as well as mass of the working substance crosses the boundary of the system
Neither the heat and work nor the mass of the working substance crosses the boundary of the system
Increases
Decreases
First increases and then decreases
First decreases and then increases
Isothermal process
Hyperbolic process
Adiabatic process
Polytropic process
Less than
Equal to
More than
None of these
Volume
Temperature
Mass
Energy
Wood
Coke
Anthracite coal
Pulverised coal
Maximum cycle temperature
Minimum cycle temperature
Pressure ratio
All of these
Equal to
Directly proportional to
Inversely proportional to
None of these
Dual combustion cycle
Diesel cycle
Atkinson cycle
Rankine cycle
Ru × T
1.5 Ru × T
2 Ru × T
3 Ru × T
Wood charcoal
Bituminous coke
Pulverised coal
Coke
Ultimate shear stress of the column
Factor of safety
Torque resisting capacity
Slenderness ratio
Shear modulus
Section modulus
Polar modulus
None of these
Resilience
Proof resilience
Strain energy
Impact energy
Plastic limit
Elastic limit
Yield point
Limit of proportionality
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
30 kJ
54 kJ
84 kJ
114 kJ
The product of the gas constant and the molecular mass of an ideal gas is constant
The sum of partial pressure of the mixture of two gases is sum of the two
Equal volumes of all gases, at the same temperature and pressure, contain equal number of molecules
All of the above
Zero
Minimum
Maximum
Infinity
Carbon and hydrogen
Oxygen and hydrogen
Sulphur and oxygen
Sulphur and hydrogen
Energy stored in a body when strained within elastic limits
Energy stored in a body when strained up to the breaking of the specimen maximum strain
Energy which can be stored in a body
None of the above
(p - 2d) t × σc
(p - d) t × τ
(p - d) t × σt
(2p - d) t × σt