πd²/4
πd²/16
πd3/16
πd3/32
D. πd3/32
√(KT/m)
√(2KT/m)
√(3KT/m)
√(5KT/m)
Isothermal process
Hyperbolic process
Adiabatic process
Polytropic process
Zeroth law of thermodynamics
First law of thermodynamics
Second law of thermodynamics
None of these
The axis of load
An oblique plane
At right angles to the axis of specimen
Would not occur
Two constant volume and two isentropic processes
Two constant pressure and two isentropic processes
Two constant volume and two isothermal processes
One constant pressure, one constant volume and two isentropic processes
23.97 bar
25 bar
26.03 bar
34.81 bar
Breaking stress
Fracture stress
Yield point stress
Ultimate tensile stress
OC
OP
OQ
PQ
It is impossible to construct an engine working on a cyclic process, whose sole purpose is to convert heat energy into work
It is possible to construct an engine working on a cyclic process, whose sole purpose is to convert heat energy into work
It is impossible to construct a device which operates in a cyclic process and produces no effect other than the transfer of heat from a cold body to a hot body
None of the above
Element
Compound
Atom
Molecule
(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)
T.ω watts
2π. T.ω watts
2π. T.ω/75 watts
2π. T.ω/4500 watts
Gas engine
Petrol engine
Steam engine
Reversible engine
Short columns
Long columns
Weak columns
Medium columns
Decrease in cut-off
Increase in cut-off
Constant cut-off
None of these
Isothermally
Isentropically
Polytropically
None of these
Area at the time of fracture
Original cross-sectional area
Average of (A) and (B)
Minimum area after fracture
Same as
Less than
Greater than
None of these
Half
Same amount
Double
One-fourth
Boyle's law
Charles' law
Gay-Lussac law
Joule's law
Resilience
Proof resilience
Modulus of resilience
Toughness
Double
Half
Same
None of these
5WL³/ 384EI
WL³/384EI
WL³/ 348EI
WL³/ 48EI
Change in volume to original volume
Change in length to original length
Change in cross-sectional area to original cross-sectional area
Any one of the above
There is no change in temperature
There is no change in enthalpy
There is no change in internal energy
All of these
(σx + σy)/2 + (1/2) × √[(σx - σy)² + 4 τ²xy]
(σx + σy)/2 - (1/2) × √[(σx - σy)² + 4 τ²xy]
(σx - σy)/2 + (1/2) × √[(σx + σy)² + 4 τ²xy]
(σx - σy)/2 - (1/2) × √[(σx + σy)² + 4 τ²xy]
Equal to
Less than
More than
None of these
Linear stress to lateral strain
Lateral strain to linear strain
Linear stress to linear strain
Shear stress to shear strain
Wood
Coke
Anthracite coal
Pulverised coal
Thermal efficiency
Work ratio
Avoids pollution
None of these