l/δl
δl/l
l.δl
l + δl
B. δl/l
Maximum calculated value
Minimum calculated value
Mean value
Extreme value
Inversely proportional to strain
Directly proportional to strain
Square root of strain
Equal to strain
0°C
273°C
273 K
None of these
Mono-atomic
Di-atomic
Tri-atomic
Poly-atomic
Gas engine
Petrol engine
Steam engine
Reversible engine
Calorific value
Heat energy
Lower calorific value
Higher calorific value
Fluids in motion
Breaking point
Plastic deformation of solids
Rupture stress
Carnot cycle
Bell-Coleman cycle
Rankine cycle
Stirling cycle
1 g
10 g
100 g
1000 g
1
1.4
1.45
2.3
Pitch
Back pitch
Diagonal pitch
Diametric pitch
Middle of bar
Supported end
Bottom end
None of these
Same
Double
Half
One-fourth
Isothermal
Isentropic
Polytropic
None of these
Dual combustion cycle
Diesel cycle
Atkinson cycle
Rankine cycle
E = 3K.C/(3K + C)
E = 6K.C/(3K + C)
E = 9K.C/(3K + C)
E = 12K.C/(3K + C)
Chain riveted joint
Diamond riveted joint
Crisscross riveted joint
Zigzag riveted joint
-273°C
73°C
237°C
-237°C
Sum
Difference
Product
Ratio
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
Greater than
Less than
Equal to
None of these
More
Less
Same
More/less depending on composition
The heat and work are boundary phenomena
The heat and work represent the energy crossing the boundary of the system
The heat and work are path functions
All of the above
Young's modulus
Bulk modulus
Modulus of rigidity
Poisson's ratio
There is no change in temperature
There is no change in enthalpy
There is no change in internal energy
All of these
Reversible cycles
Irreversible cycles
Semi-reversible cycles
Quasi-static cycles
8/3
11/3
11/7
7/3
Pressure exerted by the gas
Volume occupied by the gas
Temperature of the gas
All of these
Cracking
Carbonisation
Fractional distillation
Full distillation
Decrease in cut-off
Increase in cut-off
Constant cut-off
None of these