Specific heat at constant volume
Specific heat at constant pressure
kilo-Joule
None of these
C. kilo-Joule
Kh > Ks
Kh < Ks
Kh = Ks
None of these
Malleability
Ductility
Plasticity
Elasticity
Mass of oxygen in 1 kg of flue gas to the mass of oxygen in 1 kg of fuel
Mass of oxygen in 1 kg of fuel to the mass of oxygen in 1 kg of flue gas
Mass of carbon in 1 kg of flue gas to the mass of carbon in 1 kg of fuel
Mass of carbon in 1 kg of fuel to the mass of carbon in 1 kg of flue gas
Load/original cross-sectional area and change in length/original length
Load/ instantaneous cross-sectional area and loge (original area/ instantaneous area)
Load/ instantaneous cross-sectional area and change in length/ original length
Load/ instantaneous area and instantaneous area/original area
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
Very low
Low
High
Very high
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
log (p1p2)/log (v1v2)
log (p2/ p1)/log (v1/ v2)
log (v1/ v2)/ log (p1/p2)
log [(p1v1)/(p2v2)]
Shear force changes sign
Bending moment changes sign
Shear force is maximum
Bending moment is maximum
Enthalpy
Internal energy
Entropy
External energy
0.5 s.l.σt
s.l.σt
√2 s.l.σt
2.s.l.σt
Its temperature increases but volume decreases
Its volume increases but temperature decreases
Both temperature and volume increases
Both temperature and volume decreases
Resilience
Proof resilience
Strain energy
Impact energy
Molecular mass of the gas and the gas constant
Atomic mass of the gas and the gas constant
Molecular mass of the gas and the specific heat at constant pressure
Molecular mass of the gas and the specific heat at constant volume
Isothermal expansion
Isentropic expansion
Isothermal compression
Isentropic compression
300° to 500°C
500° to 700°C
700° to 900°C
900° to 1100°C
Equal to one
Less than one
Greater than one
None of these
0.01 to 0.1
0.23 to 0.27
0.25 to 0.33
0.4 to 0.6
√(KT/m)
√(2KT/m)
√(3KT/m)
√(5KT/m)
Becomes constant
Starts decreasing
Increases without any increase in load
None of the above
1
1.4
1.67
1.87
Peat
Lignite
Bituminous coal
Anthracite coal
Zero
Minimum
Maximum
Positive
WD3n/Cd⁴
2WD3n/Cd⁴
4WD3n/Cd⁴
8WD3n/Cd⁴
Swept volume to total volume
Total volume to swept volume
Swept volume to clearance volume
Total volume to clearance volume
Conservation of heat
Conservation of momentum
Conservation of mass
Conservation of energy
Boyle's law
Charle's law
Gay-Lussac law
Joule's law
l/δl
δl/l
l.δl
l + δl
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.
Maximum cycle temperature
Minimum cycle temperature
Pressure ratio
All of these