Always in single shear
Always in double shear
Either in single shear or double shear
None of these
B. Always in double shear
400 MPa
500 MPa
900 MPa
1400 MPa
Ultimate shear stress of the column
Factor of safety
Torque resisting capacity
Slenderness ratio
The indirect heat exchanger and cooler is avoided
Direct combustion system is used
A condenser is used
All of the above
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
Soft coal
Hard coal
Pulverised coal
Bituminous coal
(p - 2d) t × σc
(p - d) t × τ
(p - d) t × σt
(2p - d) t × σt
Young's modulus
Modulus of rigidity
Bulk modulus
Poisson's ratio
0°C
273°C
273 K
None of these
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
Equal
Proportional to their respective moduli of elasticity
Inversely proportional to their moduli of elasticity
Average of the sum of moduli of elasticity
Boyle's law
Charles' law
Gay-Lussac law
All of these
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
1
1.4
1.67
1.87
Increases power output
Improves thermal efficiency
Reduces exhaust temperature
Do not damage turbine blades
√(KT/m)
√(2KT/m)
√(3KT/m)
√(5KT/m)
Total internal energy of a system during a process remains constant
Total energy of a system remains constant
Workdone by a system is equal to the heat transferred by the system
Internal energy, enthalpy and entropy during a process remain constant
Rankine
Stirling
Carnot
Brayton
Short column
Long column
Weak column
Medium column
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
Equal to
Less than
Greater than
None of these
Plasticity
Ductility
Elasticity
Malleability
Equal to
One-half
Twice
Four times
Conservation of heat
Conservation of momentum
Conservation of mass
Conservation of energy
Increasing the highest temperature
Decreasing the highest temperature
Increasing the lowest temperature
Keeping the lowest temperature constant
Carnot cycle
Stirling cycle
Otto cycle
None of these
Creeping
Yielding
Breaking
Plasticity
Specific heat at constant volume
Specific heat at constant pressure
kilo-Joule
None of these
Same
Twice
Four times
Eight times
t
2t
4t
8t
Its temperature will increase
Its volume will increase
Both temperature and volume will increase
Neither temperature not volume will increase