Principal stresses
Normal stresses on planes at 45°
Shear stresses on planes at 45°
Normal and shear stresses on a plane
B. Normal stresses on planes at 45°
(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)
Wood charcoal
Bituminous coke
Pulverised coal
Coke
The liquid fuels consist of hydrocarbons.
The liquid fuels have higher calorific value than solid fuels.
The solid fuels have higher calorific value than liquid fuels.
A good fuel should have low ignition point.
Law of equipartition of energy
Law of conservation of energy
Law of degradation of energy
None of these
Rankine
Stirling
Carnot
Brayton
Measure shear strain
Measure linear strain
Measure volumetric strain
Relieve strain
Tensile strain increases more quickly
Tensile strain decreases more quickly
Tensile strain increases in proportion to the stress
Tensile strain decreases in proportion to the stress
When coal is first dried and then crushed to a fine powder by pulverising machine
From the finely ground coal by moulding under pressure with or without a binding material
When coal is strongly heated continuously for 42 to 48 hours in the absence of air in a closed vessel
By heating wood with a limited supply of air to a temperature not less than 280°C
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
Boyle's law
Charles' law
Gay-Lussac law
Joule's law
Cracking
Carbonisation
Fractional distillation
Full distillation
wl/6
wl/3
wl
2wl/3
External energy
Internal energy
Kinetic energy
Molecular energy
Equal to
Less than
Greater than
None of these
Tension in the masonry of the dam and its base
Overturning of the dam
Crushing of masonry at the base of the dam
Any one of the above
Reversible
Irreversible
Reversible or irreversible
None of these
Pressure and temperature
Temperature and volume
Heat and work
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]
Constant volume process
Adiabatic process
Constant pressure process
Isothermal process
Mild steel
Cast iron
Concrete
Bone of these
There is no change in temperature
There is no change in enthalpy
There is no change in internal energy
All of these
Creeping
Yielding
Breaking
Plasticity
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
0.287 J/kgK
2.87 J/kgK
28.7 J/kgK
287 J/kgK
Always in single shear
Always in double shear
Either in single shear or double shear
None of these
Equal to
Less than
More than
None of these
More
Less
Same
More/less depending on composition
Short columns
Long columns
Weak columns
Medium columns
Carnot cycle can't work with saturated steam
Heat is supplied to water at temperature below the maximum temperature of the cycle
A Rankine cycle receives heat at two places
Rankine cycle is hypothetical
Gas engine
Petrol engine
Steam engine
Reversible engine