p.v = constant, if T is kept constant
v/T = constant, if p is kept constant
p/T = constant, if v is kept constant
T/p = constant, if v is kept constant
B. v/T = constant, if p is kept constant
3/7
7/3
11/3
3/11
Not deform
Be safest
Stretch
Not stretch
(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]
0.224 litres
2.24 litres
22.4 litres
224 litres
Increases
Decreases
First increases and then decreases
First decreases and then increases
Lap joint
Butt joint
Single riveted single cover butt joint
Double riveted double cover butt joint
Fixed at both ends
Fixed at one end and free at the other end
Supported on more than two supports
Extending beyond the supports
E = 3K.C/(3K + C)
E = 6K.C/(3K + C)
E = 9K.C/(3K + C)
E = 12K.C/(3K + C)
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
Zeroth
First
Second
Third
Gauge pressure = Absolute pressure + Atmospheric pressure
Absolute pressure = Gauge pressure + Atmospheric pressure
Absolute pressure = Gauge pressure - Atmospheric pressure
Atmospheric pressure = Absolute pressure + Gauge pressure
Its temperature increases but volume decreases
Its volume increases but temperature decreases
Both temperature and volume increases
Both temperature and volume decreases
237°C
-273°C
-237°C
273°C
Boyle's law
Charles' law
Gay-Lussac law
All of these
Resilience
Proof resilience
Modulus of resilience
Toughness
(p2/p1)γ - 1/ γ
(p1/p2)γ - 1/ γ
(v2/v1)γ - 1/ γ
(v1/v2)γ - 1/ γ
3 to 6
5 to 8
10 to 20
15 to 30
Fixed at both ends
Fixed at one end and free at the other end
Supported at its ends
Supported on more than two supports
Ultimate shear stress of the column
Factor of safety
Torque resisting capacity
Slenderness ratio
8/3
11/3
11/7
7/3
Brayton cycle
Joule cycle
Carnot cycle
Reversed Brayton cycle
Q1 - 2 = dU + W1 - 2
Q1 - 2 = dU - W1 - 2
Q1 - 2 = dU/W1 - 2
Q1 - 2 = dU × W1 - 2
Sum
Difference
Multiplication
None of the above
Before point A
Beyond point A
Between points A and D
Between points D and E
Law of equipartition of energy
Law of conservation of energy
Law of degradation of energy
None of these
-100 MPa
250 MPa
300 MPa
400 MPa
In tension
In compression
Neither in tension nor in compression
None of these
Dual combustion cycle
Diesel cycle
Atkinson cycle
Rankine cycle
Brown coal
Peat
Coking bituminous coal
Non-coking bituminous coal
τ²/ 2G × Volume of shaft
τ/ 2G × Volume of shaft
τ²/ 4G × Volume of shaft
τ/ 4G × Volume of shaft