Change
Do not change
Both (A) and (B)
None of these
B. Do not change
Same
Double
Half
Four times
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
One-half
One-third
Two-third
Three-fourth
T.ω watts
2π. T.ω watts
2π. T.ω/75 watts
2π. T.ω/4500 watts
δQ = T.ds
δQ = T/ds
dQ = ds/T
None of these
Increases
Decreases
First increases and then decreases
First decreases and then increases
Mechanical and fluid friction
Unrestricted expansion
Heat transfer with a finite temperature difference
All of the above
The indirect heat exchanger and cooler is avoided
Direct combustion system is used
A condenser is used
All of the above
Yield point
Limit of proportionality
Breaking point
Elastic limit
Gauge pressure = Absolute pressure + Atmospheric pressure
Absolute pressure = Gauge pressure + Atmospheric pressure
Absolute pressure = Gauge pressure - Atmospheric pressure
Atmospheric pressure = Absolute pressure + Gauge pressure
5WL³/ 384EI
WL³/384EI
WL³/ 348EI
WL³/ 48EI
Two constant volume and two isentropic
Two constant pressure and two isentropic
Two constant volume and two isothermal
One constant pressure, one constant volume and two isentropic
Elastic limit
Yield stress
Ultimate stress
Breaking stress
Reversible cycles
Irreversible cycles
Semi-reversible cycles
Adiabatic irreversible cycles
Chain riveted joint
Diamond riveted joint
Crisscross riveted joint
Zigzag riveted joint
12
14
16
32
Butt joint
Lap joint
Double riveted lap joints
All types of joints
A right angled triangle
An isosceles triangle
An equilateral triangle
A rectangle
One right angled triangle
Two right angled triangles
One equilateral triangle
Two equilateral triangles
Straight line formula
Eulers formula
Rankines formula
Secant formula
Bearing stresses
Fatigue stresses
Crushing stresses
Resultant stresses
Carnot
Ericsson
Stirling
None of the above
3 to 6
5 to 8
15 to 20
20 to 30
Tensile in both the material
Tensile in steel and compressive in copper
Compressive in steel and tensile in copper
Compressive in both the materials
Plastic limit
Elastic limit
Yield point
Limit of proportionality
Strain energy
Resilience
Proof resilience
Impact energy
External energy
Internal energy
Kinetic energy
Molecular energy
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
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
Isochoric process
Isobaric process
Hyperbolic process
All of these