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
B. The amount of heat required to raise the temperature of unit mass of gas through one degree, at constant volume
Increasing the internal energy of gas
Doing some external work
Increasing the internal energy of gas and also for doing some external work
None of the above
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
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
e (1 - 2m)
e (1 - 2/m)
e (m - 2)
e (2/m - 1)
Temperature limits
Pressure ratio
Compression ratio
Cut-off ratio and compression ratio
Steel
Copper
Aluminium
None of the above
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.
(p - 2d) t × σc
(p - d) t × τ
(p - d) t × σt
(2p - d) t × σt
Doubled
Halved
Becomes four times
None of the above
Bearing stresses
Fatigue stresses
Crushing stresses
Resultant stresses
The indirect heat exchanger and cooler is avoided
Direct combustion system is used
A condenser is used
All of the above
8.314 J/kg mole-K
83.14 J/kgmole-K
831.4 J/kgmole-K
8314 J/kgmole-K
d/4
d/8
d/12
d/16
Wood charcoal
Bituminous coke
Pulverised coal
Coke
No heat enters or leaves the gas
The temperature of the gas changes
The change in internal energy is equal to the mechanical workdone
All of the above
Strains
Stress and strain
Shear stress and shear strain
Moduli and elasticity
Its temperature increases but volume decreases
Its volume increases but temperature decreases
Both temperature and volume increases
Both temperature and volume decreases
Cracking
Carbonisation
Fractional distillation
Full distillation
30 kJ
54 kJ
84 kJ
114 kJ
Before point A
Beyond point A
Between points A and D
Between points D and E
Ru × T
1.5 Ru × T
2 Ru × T
3 Ru × T
Energy stored in a body when strained within elastic limits
Energy stored in a body when strained up to the breaking of the specimen maximum strain
Energy which can be stored in a body
None of the above
Vapour
Perfect gas
Air
Steam
Gauge pressure = Absolute pressure + Atmospheric pressure
Absolute pressure = Gauge pressure + Atmospheric pressure
Absolute pressure = Gauge pressure - Atmospheric pressure
Atmospheric pressure = Absolute pressure + Gauge pressure
1 : 2
1 : 3
1 : 4
1 : 2.5
Heat and work crosses the boundary of the system, but the mass of the working substance does not crosses the boundary of the system
Mass of the working substance crosses the boundary of the system but the heat and work does not crosses the boundary of the system
Both the heat and work as well as mass of the working substance crosses the boundary of the system
Neither the heat and work nor the mass of the working substance crosses the boundary of the system
Top layer
Bottom layer
Neutral axis
Every cross-section
The shaft 'B' has the greater diameter
The shaft 'A' has the greater diameter
Both are of same diameter
None of these
Carnot
Ericsson
Stirling
None of the above
Coal gas
Producer gas
Mond gas
Blast furnace gas