Ultimate shear stress of the column
Factor of safety
Torque resisting capacity
Slenderness ratio
D. Slenderness ratio
Zeroth law of thermodynamics
First law of thermodynamics
Second law of thermodynamics
None of these
log (p1p2)/log (v1v2)
log (p2/ p1)/log (v1/ v2)
log (v1/ v2)/ log (p1/p2)
log [(p1v1)/(p2v2)]
The first row
The second row
The central row
One rivet hole of the end row
Same as
Less than
Greater than
None of these
All the reversible engines have the same efficiency.
All the reversible and irreversible engines have the same efficiency.
Irreversible engines have maximum efficiency.
All engines are designed as reversible in order to obtain maximum efficiency.
Hookes law
Yield point
Plastic flow
Proof stress
Carnot cycle
Bell-Coleman cycle
Rankine cycle
Stirling cycle
Equal to
More than
Less than
None of these
2
8
16
32
Mechanical and fluid friction
Unrestricted expansion
Heat transfer with a finite temperature difference
All of the above
Cut-off is increased
Cut-off is decreased
Cut-off is zero
Cut-off is constant
More
Less
Equal
Depends on other factors
Increases the internal energy of the gas
Increases the temperature of the gas
Does some external work during expansion
Both (B) and (C)
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
Not deform
Be safest
Stretch
Not stretch
The indirect heat exchanger and cooler is avoided
Direct combustion system is used
A condenser is used
All of the above
Longitudinal stress to longitudinal strain
Volumetric stress to volumetric strain
Lateral stress to Lateral strain
Shear stress to shear strain
Element
Compound
Atom
Molecule
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
2ε₁ - ε₂
2ε₁ + ε₂
2ε₂ - ε₁
2ε₂ + ε₁
Equal to
One-half
Twice
Four times
Constant volume
Constant temperature
Constant pressure
None of these
Greater than
Less than
Equal to
None of these
Bearing stresses
Fatigue stresses
Crushing stresses
Resultant stresses
4 tonnes/ cm²
8 tonnes/ cm²
16 tonnes/ cm²
22 tonnes/ cm²
Equal to
Less than
More than
None of these
1/8
1/4
1/2
2
Joule (J)
Joule metre (Jm)
Watt (W)
Joule/metre (J/m)
Axis of load
Perpendicular to the axis of load
Maximum moment of inertia
Minimum moment of inertia
Carnot
Ericsson
Stirling
None of the above