Steel only
Concrete only
Steel and concrete both
None of these
C. Steel and concrete both
Straight line formula
Eulers formula
Rankines formula
Secant formula
Equal to
Directly proportional to
Inversely proportional to
None of these
Coke
Wood charcoal
Bituminous coal
Briquetted coal
Linear stress to lateral strain
Lateral strain to linear strain
Linear stress to linear strain
Shear stress to shear strain
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
(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)
Strain energy
Resilience
Proof resilience
Impact energy
Remains constant
Decreases
Increases
None of these
12
14
16
32
Change
Do not change
Both (A) and (B)
None of these
Kelvin
Joule
Clausis
Gay-Lussac
Short columns
Long columns
Both short and long columns
Weak columns
Remains constant
Increases
Decreases
None of these
Element
Compound
Atom
Molecule
0.086
1.086
1.086
4.086
Zero
Minimum
Maximum
Positive
Temperature limits
Pressure ratio
Volume compression ratio
Cut-off ratio and compression ratio
cv/ cp =R
cp - cv = R
cv = R/ γ-1
Both (B) and (C)
Short column
Long column
Weak column
Medium column
Volumetric stress and volumetric strain
Lateral stress and lateral strain
Longitudinal stress and longitudinal strain
Shear stress to shear strain
Greater than
Less than
Equal to
None of these
30 MN/m²
50 MN/m²
100 MN/m²
200 MN/m²
Doubled
Halved
Becomes four times
None of the above
Maximum cycle temperature
Minimum cycle temperature
Pressure ratio
All of these
Carnot
Ericsson
Stirling
None of the above
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
Boyle's law
Charle's law
Gay-Lussac law
Joule's law
Conservation of heat
Conservation of momentum
Conservation of mass
Conservation of energy
T.ω watts
2π. T.ω watts
2π. T.ω/75 watts
2π. T.ω/4500 watts
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.