Isochoric process
Isobaric process
Hyperbolic process
All of these
D. All of these
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
Greater than Diesel cycle and less than Otto cycle
Less than Diesel cycle and greater than Otto cycle
Greater than Diesel cycle
Less than Diesel cycle
Increasing the highest temperature
Decreasing the highest temperature
Increasing the lowest temperature
Keeping the lowest temperature constant
Two constant volume and two isentropic processes
Two constant pressure and two isentropic processes
Two constant volume and two isothermal processes
One constant pressure, one constant volume and two isentropic processes
65° to 220°C
220° to 345°C
345° to 470°C
470° to 550°C
Carnot cycle
Otto cycle
Joule's cycle
Stirling cycle
Pressure
Volume
Temperature
All of these
Peat
Lignite
Bituminous coal
Anthracite coal
Constant pressure cycle
Constant volume cycle
Constant temperature cycle
Constant temperature and pressure cycle
Constant pressure process
Constant volume process
Constant pvn process
All of these
Tension
Compression
Bearing
Any one of the above
Breaking stress
Fracture stress
Yield point stress
Ultimate tensile stress
Equal to
Less than
More than
None of these
Remains constant
Increases
Decreases
None of these
50 %
25 %
0 %
15 %
No stress
Shear stress
Tensile stress
Compressive stress
Boyle's law
Charles' law
Gay-Lussac law
Avogadro's law
Strains
Stress and strain
Shear stress and shear strain
Moduli and elasticity
mm/mm
kg/cm
Kg
kg/cm²
Acts at a point on a beam
Spreads non-uniformly over the whole length of a beam
Spreads uniformly over the whole length of a beam
Varies uniformly over the whole length of a beam
(σx + σy)/2 + (1/2) × √[(σx - σy)² + 4 τ²xy]
(σx + σy)/2 - (1/2) × √[(σx - σy)² + 4 τ²xy]
(σx - σy)/2 + (1/2) × √[(σx + σy)² + 4 τ²xy]
(σx - σy)/2 - (1/2) × √[(σx + σy)² + 4 τ²xy]
Fixed at both ends
Fixed at one end and free at the other end
Supported on more than two supports
Extending beyond the supports
Total internal energy of a system during a process remains constant
Total energy of a system remains constant
Workdone by a system is equal to the heat transferred by the system
Internal energy, enthalpy and entropy during a process remain constant
Less than
Equal to
More than
None of these
Same
More
Less
Unpredictable
Lap joint
Butt joint
Single riveted single cover butt joint
Double riveted double cover butt joint
Q1 - 2 = dU + W1 - 2
Q1 - 2 = dU - W1 - 2
Q1 - 2 = dU/W1 - 2
Q1 - 2 = dU × W1 - 2
Zero
Minimum
Maximum
Infinity
Rubber
Plastic
Brass
Steel
Soft coal
Hard coal
Pulverised coal
Bituminous coal