Unit mass
Modulus of rigidity
Bulk modulus
Modulus of Elasticity
D. Modulus of Elasticity
Greater than
Less than
Equal to
None of these
Carnot
Ericsson
Stirling
None of the above
Bending moment (i.e. M)
Bending moment² (i.e. M²)
Bending moment³ (i.e. M³)
Bending moment⁴ (i.e. M⁴)
Two constant pressure
Two constant volume
Two isentropic
One constant pressure, one constant volume
1/8
1/4
1/2
2
10 MPa
30 MPa
50 MPa
100 MPa
Otto cycle
Ericsson cycle
Joule cycle
Stirling cycle
Before point A
Beyond point A
Between points A and D
Between points D and E
Two constant volume and two isentropic processes
Two isothermal and two isentropic processes
Two constant pressure and two isentropic processes
One constant volume, one constant pressure and two isentropic processes
Constant volume
Constant temperature
Constant pressure
None of these
T.ω watts
2π. T.ω watts
2π. T.ω/75 watts
2π. T.ω/4500 watts
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
800 K
1000 K
1200 K
1400 K
Yield point stress
Breaking stress
Ultimate stress
Elastic limit
Young's modulus
Bulk modulus
Modulus of rigidity
Poisson's ratio
1 N-m/s
100 N-m
1000 N-m/s
1 × 106 N-m/s
Its temperature will increase
Its pressure will increase
Both temperature and pressure will increase
Neither temperature nor pressure will increase
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
The stress is the pressure per unit area
The strain is expressed in mm
Hook's law holds good upto the breaking point
Stress is directly proportional to strain within elastic limit
Conservation of work
Conservation of heat
Conversion of heat into work
Conversion of work into heat
Loss of heat
No loss of heat
Gain of heat
No gain of heat
Conservation of heat
Conservation of momentum
Conservation of mass
Conservation of energy
50 %
25 %
0 %
15 %
Plasticity
Elasticity
Ductility
Malleability
Remains constant
Increases
Decreases
None of these
0
1
γ
∝
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
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
Joint less section
Homogeneous section
Perfect section
Seamless section
400 MPa
500 MPa
900 MPa
1400 MPa