More
Less
Equal
Depends on other factors
C. Equal
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
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
Tension in the masonry of the dam and its base
Overturning of the dam
Crushing of masonry at the base of the dam
Any one of the above
Boyle's law
Charles' law
Gay-Lussac law
Avogadro's law
Carnot cycle
Stirling cycle
Otto cycle
None of these
L = l/2
L = l/√2
L = l
L = 2l
Molecular mass of the gas and the specific heat at constant volume
Atomic mass of the gas and the gas constant
Molecular mass of the gas and the gas constant
None of the above
Law of equipartition of energy
Law of conservation of energy
Law of degradation of energy
None of these
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
Fixed at both ends
Fixed at one end and free at the other end
Supported at its ends
Supported on more than two supports
Constant pressure cycle
Constant volume cycle
Constant temperature cycle
Constant temperature and pressure cycle
Isothermal process
Hyperbolic process
Adiabatic process
Polytropic process
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
Elastic limit
Yield stress
Ultimate stress
Breaking stress
30 MN/m²
50 MN/m²
100 MN/m²
200 MN/m²
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
Specific heat at constant volume
Specific heat at constant pressure
Kilo Joule
None of these
Elastic point of the material
Plastic point of the material
Breaking point of the material
Yielding point of the material
0°
30°
45°
90°
Two constant volume and two isentropic
Two constant pressure and two isentropic
Two constant volume and two isothermal
One constant pressure, one constant volume and two isentropic
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.
Same
More
Less
Unpredictable
Peat
Lignite
Bituminous coal
Anthracite coal
Malleability
Ductility
Plasticity
Elasticity
Fixed at both ends
Fixed at one end and free at the other end
Supported on more than two supports
Extending beyond the supports
Maximum shear stress
No shear stress
Minimum shear stress
None of the above
Joint less section
Homogeneous section
Perfect section
Seamless section
Oxygen
Nitrogen
Hydrogen
Methane
Sum
Difference
Product
Ratio
Fluids in motion
Breaking point
Plastic deformation of solids
Rupture stress