WD3n/Cd⁴
2WD3n/Cd⁴
4WD3n/Cd⁴
8WD3n/Cd⁴
D. 8WD3n/Cd⁴
Straight line formula
Eulers formula
Rankines formula
Secant formula
Young's modulus
Bulk modulus
Modulus of rigidity
Modulus of elasticity
Pressure
Volume
Temperature
Density
Thermodynamic law
Thermodynamic process
Thermodynamic cycle
None of these
0
1
γ
∝
mR (T2 - T1)
mcv (T2 - T1)
mcp (T2 - T1)
mcp (T2 + T1)
Very low
Low
High
Very high
Permanent
Temporary
Semi-permanent
None of these
1
1.4
1.45
2.3
Isothermal process
Hyperbolic process
Adiabatic process
Polytropic process
12
14
16
32
Ultimate shear stress of the column
Factor of safety
Torque resisting capacity
Slenderness ratio
From maximum at the centre to zero at the circumference
From zero at the centre to maximum at the circumference
From maximum at the centre to minimum at the circumference
From minimum at the centre to maximum at the circumference
(p2/p1)γ - 1/ γ
(p1/p2)γ - 1/ γ
(v2/v1)γ - 1/ γ
(v1/v2)γ - 1/ γ
11/7
9/7
4/7
All of the above
12
14
16
32
Pressure
Volume
Temperature
All of these
1
0
-1
10
No heat enters or leaves the gas
The temperature of the gas changes
The change in internal energy is equal to the mechanical workdone
All of the above
Sum of two principal stresses
Difference of two principal stresses
Half the sum of two principal stresses
Half the difference of two principal stresses
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
Increase in availability of energy
Increase in temperature
Decrease in pressure
Degradation of energy
Oxygen
Sulphur
Nitrogen
Carbon
Bearing stresses
Fatigue stresses
Crushing stresses
Resultant stresses
(σx/2) + (1/2) × √(σx² + 4 τ²xy)
(σx/2) - (1/2) × √(σx² + 4 τ²xy)
(σx/2) + (1/2) × √(σx² - 4 τ²xy)
(1/2) × √(σx² + 4 τ²xy)
Inversely proportional to two times
Directly proportional to
Inversely proportional to
None of these
Dual combustion cycle
Diesel cycle
Atkinson cycle
Rankine cycle
Smaller end
Larger end
Middle
Anywhere
(m - 1)/ (2m - 1)
(2m - 1)/ (m - 1)
(m - 2)/ (3m - 4)
(m - 2)/ (5m - 4)
Constant volume process
Adiabatic process
Constant pressure process
Isothermal process