Its temperature increases but volume decreases
Its volume increases but temperature decreases
Both temperature and volume increases
Both temperature and volume decreases
D. Both temperature and volume decreases
30 kJ
54 kJ
84 kJ
114 kJ
Equal to
One-half
Twice
Four times
Carnot
Stirling
Ericsson
None of the above
Joule (J)
Joule metre (Jm)
Watt (W)
Joule/metre (J/m)
Oxygen
Nitrogen
Hydrogen
Methane
Carnot cycle
Otto cycle
Joule's cycle
Stirling cycle
0.4 radian
0.8 radian
1.6 radian
3.2 radian
Carnot cycle
Bell-Coleman cycle
Rankine cycle
Stirling cycle
Element
Compound
Atom
Molecule
Equal to
Less than
More than
None of these
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
Constant pressure cycle
Constant volume cycle
Constant temperature cycle
Constant temperature and pressure cycle
Peat
Lignite
Bituminous coal
Anthracite coal
Petrol engine
Diesel engine
Reversible engine
Irreversible engine
Zero
Minimum
Maximum
Infinity
Tensile stress
Compressive stress
Shear stress
Strain
Working substance
Design of engine
Size of engine
Temperatures of source and sink
2
8
16
32
3p/E × (2/m - 1)
3p/E × (2 - m)
3p/E × (1 - 2/m)
E/3p × (2/m - 1)
Sum
Difference
Multiplication
None of the above
It is possible to transfer heat from a body at a lower temperature to a body at a higher temperature.
It is impossible to transfer heat from a body at a lower temperature to a body at a higher temperature, without the aid of an external source.
It is possible to transfer heat from a body at a lower temperature to a body at a higher temperature by using refrigeration cycle.
None of the above
Law of equipartition of energy
Law of conservation of energy
Law of degradation of energy
None of these
Energy stored in a body when strained within elastic limits
Energy stored in a body when strained up to the breaking of a specimen
Maximum strain energy which can be stored in a body
Proof resilience per unit volume of a material
Wl3/48 EI
Wa²b²/3EIl
[Wa/(a√3) x EIl] x (l² - a²)3/2
5Wl3/384 EI
Increase key length
Increase key depth
Increase key width
Double all the dimensions
Principal stress
Tensile stress
Compressive stress
Shear stress
1.817
2512
4.187
None of these
Tensile
Compressive
Shear
Zero
Combustion is at constant volume
Expansion and compression are isentropic
Maximum temperature is higher
Heat rejection is lower
wl/6
wl/3
wl
2wl/3