Zero
Minimum
Maximum
Infinity
C. Maximum
Dual combustion cycle
Diesel cycle
Atkinson cycle
Rankine cycle
Carbon
Hydrogen and nitrogen
Sulphur and ash
All of these
Young's modulus
Bulk modulus
Modulus of rigidity
Poisson's ratio
K₁ K₂
(K₁ + K₂)/ 2
(K₁ + K₂)/ K₁ K₂
K₁ K₂/ (K₁ + K₂)
Straight line formula
Eulers formula
Rankines formula
Secant formula
9/7
11/7
7/4
1/4
Equal to
Half
Double
Quadruple
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
Plasticity
Elasticity
Ductility
Malleability
Reversible process
Irreversible process
Reversible or irreversible process
None of these
Tensile
Compressive
Shear
Zero
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
Smaller end
Larger end
Middle
Anywhere
Element
Compound
Atom
Molecule
Very low
Low
High
Very high
Fixed at both ends
Fixed at one end and free at the other end
Supported at its ends
Supported on more than two supports
Equal to
Less than
More than
None of these
Radius
Diameter
Circumference
Area
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
Increases the internal energy of the gas
Increases the temperature of the gas
Does some external work during expansion
Both (B) and (C)
Constant volume process
Adiabatic process
Constant pressure process
Isothermal process
Linear stress to linear strain
Linear stress to lateral strain
Volumetric strain to linear strain
Shear stress to shear strain
Carnot cycle
Bell-Coleman cycle
Rankine cycle
Stirling cycle
Yield point stress
Breaking stress
Ultimate stress
Elastic limit
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
More
Less
Equal
Depends on other factors
Carnot
Ericsson
Stirling
None of the above
Shear modulus
Section modulus
Polar modulus
None of these
Zero
Minimum
Maximum
Positive
Remains constant
Decreases
Increases
None of these