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
D. None of the above
e (1 - 2m)
e (1 - 2/m)
e (m - 2)
e (2/m - 1)
Of same magnitude as that of bar and applied at the lower end
Half the weight of bar applied at lower end
Half of the square of weight of bar applied at lower end
One fourth of weight of bar applied at lower end
Always in single shear
Always in double shear
Either in single shear or double shear
None of these
400 MPa
500 MPa
900 MPa
1400 MPa
1
1.4
1.45
2.3
Same torque
Less torque
More torque
Unpredictable
Maximum torque it can transmit
Number of cycles it undergoes before failure
Elastic limit up to which it resists torsion, shear and bending stresses
Torque required to produce a twist of one radian per unit length of shaft
1/8
1/4
1/2
2
Ultimate shear stress of the column
Factor of safety
Torque resisting capacity
Slenderness ratio
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
Same
Double
Half
One-fourth
Boyle's law
Charles' law
Gay-Lussac law
Avogadro's law
Two isothermals and two isentropic
Two isentropic and two constant volumes
Two isentropic, one constant volume and one constant pressure
Two isentropic and two constant pressures
More
Less
Equal
Depends on other factors
Extensive heat is transferred
Extensive work is done
Extensive energy is utilised
None of these
L = l/2
L = l/√2
L = l
L = 2l
Two isothermals and two isentropic
Two isentropic and two constant volumes
Two isentropic, one constant volume and one constant pressure
Two isentropic and two constant pressures
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
(T1/T2) - 1
1 - (T1/T2)
1 - (T2/T1)
1 + (T2/T1)
Vapour
Perfect gas
Air
Steam
Sum of two specific heats
Difference of two specific heats
Product of two specific heats
Ratio of two specific heats
Carnot cycle
Stirling cycle
Otto cycle
None of these
Boyle's law
Charles' law
Gay-Lussac law
Avogadro's law
For a given compression ratio, both Otto and Diesel cycles have the same efficiency.
For a given compression ratio, Otto cycle is more efficient than Diesel cycle.
For a given compression ratio, Diesel cycle is more efficient than Otto cycle.
The efficiency of Otto or Diesel cycle has nothing to do with compression ratio.
Conservation of heat
Conservation of momentum
Conservation of mass
Conservation of energy
Conservation of work
Conservation of heat
Conversion of heat into work
Conversion of work into heat
Plasticity
Elasticity
Ductility
Malleability
Linear stress to linear strain
Linear stress to lateral strain
Volumetric strain to linear strain
Shear stress to shear strain
Wl3 / 48EI
5Wl3 / 384EI
Wl3 / 392EI
Wl3 / 384EI
Thermal efficiency
Work ratio
Avoids pollution
None of these