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
A. Energy stored in a body when strained within elastic limits
Working substance
Design of engine
Size of engine
Temperatures of source and sink
0.01 to 0.1
0.23 to 0.27
0.25 to 0.33
0.4 to 0.6
Increases power output
Improves thermal efficiency
Reduces exhaust temperature
Do not damage turbine blades
Zeroth law of thermodynamics
First law of thermodynamics
Second law of thermodynamics
Kelvin Planck's law
Otto cycle
Ericsson cycle
Joule cycle
Stirling cycle
(p - 2d) t × σc
(p - d) t × τ
(p - d) t × σt
(2p - d) t × σt
0.224 litres
2.24 litres
22.4 litres
224 litres
Elastic point of the material
Plastic point of the material
Breaking point of the material
Yielding point of the material
Carnot
Ericsson
Stirling
None of the above
Specific heat at constant volume
Specific heat at constant pressure
Kilo Joule
None of these
1 g
10 g
100 g
1000 g
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
Temperature limits
Pressure ratio
Compression ratio
Cut-off ratio and compression ratio
In the middle
At the tip below the load
At the support
Anywhere
-273°C
73°C
237°C
-237°C
T.ω watts
2π. T.ω watts
2π. T.ω/75 watts
2π. T.ω/4500 watts
Remains constant
Decreases
Increases
None of these
Increases
Decreases
First increases and then decreases
First decreases and then increases
Pitch
Back pitch
Diagonal pitch
Diametric pitch
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.
Coal gas
Producer gas
Mond gas
Blast furnace gas
1/8
1/4
1/2
2
Half
Same amount
Double
One-fourth
1 kg of water
7 kg of water
8 kg of water
9 kg of water
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
Same
Half
Two times
Four times
Workdone
Entropy
Enthalpy
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
Area of cross-section of the column
Length and least radius of gyration of the column
Modulus of elasticity for the material of the column
All of the above
1.817
2512
4.187
None of these