Two constant pressure
Two constant volume
Two isentropic
One constant pressure, one constant volume
B. Two constant volume
Carnot
Stirling
Ericsson
None of the above
It is impossible to construct an engine working on a cyclic process, whose sole purpose is to convert heat energy into work.
It is impossible to transfer heat from a body at a lower temperature to a higher temperature, without the aid of an external source.
There is a definite amount of mechanical energy, which can be obtained from a given quantity of heat energy.
All of the above
Before point A
Beyond point A
Between points A and D
Between points D and E
Isothermal expansion
Isentropic expansion
Isothermal compression
Isentropic compression
Same
Half
Two times
Four times
Energy stored in a body when strained within elastic limits
Energy stored in a body when strained up to the breaking of a specimen
Maximum strain energy which can be stored in a body
Proof resilience per unit volume of a material
kJ
kJ/kg
kJ/m2
kJ/m3
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
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
Principal stress
Tensile stress
Compressive stress
Shear stress
πd²/4
πd²/16
πd3/16
πd3/32
Tensile stress
Compressive stress
Shear stress
Strain
1 : 2
1 : 3
1 : 4
1 : 2.5
l/8
l/4
l/2
l
Principal stresses
Normal stresses on planes at 45°
Shear stresses on planes at 45°
Normal and shear stresses on a plane
More than 50 %
25-50 %
10-25 %
Negligible
Extensive heat is transferred
Extensive work is done
Extensive energy is utilised
None of these
Ru × T
1.5 Ru × T
2 Ru × T
3 Ru × T
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
Slenderness ratio and area of cross-section
Poisson's ratio and modulus of elasticity
Slenderness ratio and modulus of elasticity
Slenderness ratio, area of cross-section and modulus of elasticity
Temperature limits
Pressure ratio
Compression ratio
Cut-off ratio and compression ratio
The first row
The second row
The central row
One rivet hole of the end row
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
(p2/p1)γ - 1/ γ
(p1/p2)γ - 1/ γ
(v2/v1)γ - 1/ γ
(v1/v2)γ - 1/ γ
Ultimate shear stress of the column
Factor of safety
Torque resisting capacity
Slenderness ratio
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.
Petrol engine
Diesel engine
Reversible engine
Irreversible engine
800 K
1000 K
1200 K
1400 K
Calorific value
Heat energy
Lower calorific value
Higher calorific value
Carnot cycle
Stirling cycle
Otto cycle
None of these