Half
Same amount
Double
One-fourth
B. Same amount
Thermodynamic law
Thermodynamic process
Thermodynamic cycle
None of these
Carnot cycle
Stirling cycle
Otto cycle
None of these
Ends are firmly fixed
Column is supported on all sides throughout the length
Length is equal to radius of gyration
Length is twice the radius of gyration
Thermal efficiency
Work ratio
Avoids pollution
None of these
Two constant volume and two isentropic processes
Two constant volume and two isothermal processes
Two constant pressure and two isothermal processes
One constant volume, one constant pressure and two isentropic processes
Carbon and hydrogen
Oxygen and hydrogen
Sulphur and oxygen
Sulphur and hydrogen
Short columns
Long columns
Both short and long columns
Weak columns
The liquid fuels have higher calorific value than solid fuels
The solid fuels have higher calorific value than liquid fuels
A good fuel should have low ignition point
The liquid fuels consist of hydrocarbons
Brayton cycle
Joule cycle
Carnot cycle
Reversed Brayton cycle
Petrol engine
Diesel engine
Reversible engine
Irreversible engine
Otto cycle is more efficient than Diesel cycle
Diesel cycle is more efficient than Otto cycle
Dual cycle is more efficient than Otto and Diesel cycles
Dual cycle is less efficient than Otto and Diesel cycles
1 g
10 g
100 g
1000 g
-140 kJ
-80 kJ
-40 kJ
+60 kJ
Change in volume to original volume
Change in length to original length
Change in cross-sectional area to original cross-sectional area
Any one of the above
When molecular momentum of the system becomes zero
At sea level
At the temperature of - 273 K
At the centre of the earth
Heat absorbed
Heat rejected
Either (A) or (B)
None of these
It is used as the alternate standard of comparison of all heat engines.
All the heat engines are based on Carnot cycle.
It provides concept of maximising work output between the two temperature limits.
All of the above
Otto cycle is more efficient than Diesel cycle
Diesel cycle is more efficient than Otto cycle
Efficiency depends on other factors
Both Otto and Diesel cycles are equally efficient
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
Toughness
Tensile strength
Capability of being cold worked
Hardness
Sum of two specific heats
Difference of two specific heats
Product of two specific heats
Ratio of two specific heats
3 to 6
5 to 8
15 to 20
20 to 30
Temperature limits
Pressure ratio
Compression ratio
Cut-off ratio and compression ratio
Boyle's law
Charle's law
Gay-Lussac law
Joule's law
No stress
Shear stress
Tensile stress
Compressive stress
3 to 6
5 to 8
10 to 20
15 to 30
Pressure exerted by the gas
Volume occupied by the gas
Temperature of the gas
All of these
Workdone
Entropy
Enthalpy
None of these
d/4
d/8
d/12
d/16
Boyle's law
Charles' law
Gay-Lussac law
All of these