Thermodynamic law
Thermodynamic process
Thermodynamic cycle
None of these
B. Thermodynamic process
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
Change
Do not change
Both (A) and (B)
None of these
Isothermally
Isentropically
Polytropically
None of these
Increase key length
Increase key depth
Increase key width
Double all the dimensions
Maximum calculated value
Minimum calculated value
Mean value
Extreme value
-273°C
73°C
237°C
-237°C
Elements
Compounds
Atoms
Molecules
The stress and strain induced is compressive
The stress and strain induced is tensile
Both A and B is correct
None of these
Equal to one
Less than one
Greater than one
None of these
(23/100) × Mass of excess carbon
(23/100) × Mass of excess oxygen
(100/23) × Mass of excess carbon
(100/23) × Mass of excess oxygen
Thermodynamic system
Thermodynamic cycle
Thermodynamic process
Thermodynamic law
Principal stress
Tensile stress
Compressive stress
Shear stress
Two constant volume and two isentropic processes
Two isothermal and two isentropic processes
Two constant pressure and two isentropic processes
One constant volume, one constant pressure and two isentropic processes
W1 - 2 = 0
Q1 - 2 = 0
dU = 0
All of these
Linear stress to linear strain
Linear stress to lateral strain
Volumetric strain to linear strain
Shear stress to shear strain
Equal to
Less than
Greater than
None of these
Half
Same amount
Double
One-fourth
Young's modulus
Bulk modulus
Modulus of rigidity
Modulus of elasticity
For a given compression ratio, both Otto and Diesel cycles have the same efficiency.
For a given compression ratio, Otto cycle is more efficient than Diesel cycle.
For a given compression ratio, Diesel cycle is more efficient than Otto cycle.
The efficiency of Otto or Diesel cycle has nothing to do with compression ratio.
Isothermal
Isentropic
Polytropic
None of these
p.t.σt
d.t.σc
π/4 × d² × σt
π/4 × d² × σc
Boyle's law
Charles' law
Gay-Lussac law
Avogadro's law
The amount of heat required to raise the temperature of unit mass of gas through one degree, at constant pressure
The amount of heat required to raise the temperature of unit mass of gas through one degree, at constant volume
The amount of heat required to raise the temperature of 1 kg of water through one degree
Any one of the above
More
Less
Same
More/less depending on composition
mm/mm
kg/cm
Kg
kg/cm²
e (1 - 2m)
e (1 - 2/m)
e (m - 2)
e (2/m - 1)
Greater than
Less than
Equal to
None of these
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
(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)
Sum of two specific heats
Difference of two specific heats
Product of two specific heats
Ratio of two specific heats