It is made of thick sheets
The internal pressure is very high
The ratio of wall thickness of the vessel to its diameter is less than 1/10.
The ratio of wall thickness of the vessel to its diameter is greater than 1/10.
D. The ratio of wall thickness of the vessel to its diameter is greater than 1/10.
√(KT/m)
√(2KT/m)
√(3KT/m)
√(5KT/m)
50 %
25 %
0 %
15 %
Increase key length
Increase key depth
Increase key width
Double all the dimensions
0.287 J/kgK
2.87 J/kgK
28.7 J/kgK
287 J/kgK
800 K
1000 K
1200 K
1400 K
T.ω watts
2π. T.ω watts
2π. T.ω/75 watts
2π. T.ω/4500 watts
Pressure
Volume
Temperature
All of these
Low
Very low
High
Very high
1 kg of water
7 kg of water
8 kg of water
9 kg of water
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
Maximum at periphery and zero at center
Maximum at center
Uniform throughout
None of the above
It is impossible to construct an engine working on a cyclic process, whose sole purpose is to convert heat energy into work.
It is impossible to transfer heat from a body at a lower temperature to a higher temperature, without the aid of an external source.
There is a definite amount of mechanical energy, which can be obtained from a given quantity of heat energy.
All of the above
A Joule cycle consists of two constant volume and two isentropic processes.
An Otto cycle consists of two constant volume and two isentropic processes.
An Ericsson cycle consists of two constant pressure and two isothermal processes.
All of the above
Doubled
Halved
Becomes four times
None of the above
Greater than
Less than
Equal to
None of these
Remains constant
Increases
Decreases
None of these
Increase in availability of energy
Increase in temperature
Decrease in pressure
Degradation of energy
The first row
The second row
The central row
One rivet hole of the end row
Permanent
Temporary
Semi-permanent
None of these
Frequent heat treatment
Fatigue
Creep
Shock loading
12
14
16
32
Yield point
Limit of proportionality
Breaking point
Elastic limit
Short column
Long column
Weak column
Medium column
Flow processes
Non-flow processes
Adiabatic processes
None of these
Its own length
Twice its length
Half its length
1/√2 × its length
5WL³/ 384EI
WL³/384EI
WL³/ 348EI
WL³/ 48EI
Law of equipartition of energy
Law of conservation of energy
Law of degradation of energy
None of these
mR (T2 - T1)
mcv (T2 - T1)
mcp (T2 - T1)
mcp (T2 + T1)
Petrol
Kerosene
Fuel oil
Lubricating oil
Sum of two specific heats
Difference of two specific heats
Product of two specific heats
Ratio of two specific heats