It is impossible to construct an engine working on a cyclic process, whose sole purpose is to convert heat energy into work
It is possible to construct an engine working on a cyclic process, whose sole purpose is to convert heat energy into work
It is impossible to construct a device which operates in a cyclic process and produces no effect other than the transfer of heat from a cold body to a hot body
None of the above
A. It is impossible to construct an engine working on a cyclic process, whose sole purpose is to convert heat energy into work
(p1 v1 - p2 v2)/(γ - 1)
[m R (T1 - T2)] /(γ - 1)
[m R T1/(γ - 1)][1 - (p2 v2 /p1 v1)]
All of these
Zero
Minimum
Maximum
Infinity
Thermodynamic law
Thermodynamic process
Thermodynamic cycle
None of these
Oxygen
Nitrogen
Hydrogen
Methane
Resilience
Proof resilience
Modulus of resilience
Toughness
Increases the internal energy of the gas
Increases the temperature of the gas
Does some external work during expansion
Both (B) and (C)
In tension
In compression
Neither in tension nor in compression
None of these
Mass of oxygen in 1 kg of flue gas to the mass of oxygen in 1 kg of fuel
Mass of oxygen in 1 kg of fuel to the mass of oxygen in 1 kg of flue gas
Mass of carbon in 1 kg of flue gas to the mass of carbon in 1 kg of fuel
Mass of carbon in 1 kg of fuel to the mass of carbon in 1 kg of flue gas
Wl3 / 48EI
5Wl3 / 384EI
Wl3 / 392EI
Wl3 / 384EI
Creeping
Yielding
Breaking
Plasticity
30 MN/m²
50 MN/m²
100 MN/m²
200 MN/m²
Equal
Proportional to their respective moduli of elasticity
Inversely proportional to their moduli of elasticity
Average of the sum of moduli of elasticity
Plasticity
Ductility
Elasticity
Malleability
Zeroth
First
Second
Third
l/δl
δl/l
l.δl
l + δl
Extensive heat is transferred
Extensive work is done
Extensive energy is utilised
None of these
Its temperature will increase
Its volume will increase
Both temperature and volume will increase
Neither temperature not volume will increase
0°
30°
45°
90°
The axis of load
An oblique plane
At right angles to the axis of specimen
Would not occur
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
wl/6
wl/3
wl
2wl/3
Cracking
Carbonisation
Fractional distillation
Full distillation
Boyle
Charles
Joule
None of these
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
wl/4
wl/2
wl
wl²/2
There is no change in temperature
There is no change in enthalpy
There is no change in internal energy
All of these
v1/v2
v2/v1
(v1 + v2)/v1
(v1 + v2)/v2
Carnot
Stirling
Ericsson
None of the above
Half
Same amount
Double
One-fourth
237°C
-273°C
-237°C
273°C