Shear force changes sign
Shear force is maximum
Bending moment changes sign
Bending moment is maximum
C. Bending moment changes sign
Chain riveted joint
Diamond riveted joint
Crisscross riveted joint
Zigzag riveted joint
Shear force changes sign
Shear force is maximum
Bending moment changes sign
Bending moment is maximum
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
Same
Half
Two times
Four times
Combustion is at constant volume
Expansion and compression are isentropic
Maximum temperature is higher
Heat rejection is lower
300° to 500°C
500° to 700°C
700° to 900°C
900° to 1100°C
Same
Lower
Higher
None of these
Heat absorbed
Heat rejected
Either (A) or (B)
None of these
(p2/p1)γ - 1/ γ
(p1/p2)γ - 1/ γ
(v2/v1)γ - 1/ γ
(v1/v2)γ - 1/ γ
Maximum calculated value
Minimum calculated value
Mean value
Extreme value
Reversible process
Irreversible process
Reversible or irreversible process
None of these
Young's modulus
Bulk modulus
Modulus of rigidity
Poisson's ratio
T.ω watts
2π. T.ω watts
2π. T.ω/75 watts
2π. T.ω/4500 watts
The closed cycle gas turbine plants are external combustion plants.
In the closed cycle gas turbine, the pressure range depends upon the atmospheric pressure.
The advantage of efficient internal combustion is eliminated as the closed cycle has an external surface.
In open cycle gas turbine, atmosphere acts as a sink and no coolant is required.
Elements
Compounds
Atoms
Molecules
Petrol
Kerosene
Fuel oil
Lubricating oil
Reversible cycle
Irreversible cycle
Thermodynamic cycle
None of these
Maximum shear stress
No shear stress
Minimum shear stress
None of the above
12
14
16
32
0°
30°
45°
90°
Wl3/48 EI
Wa²b²/3EIl
[Wa/(a√3) x EIl] x (l² - a²)3/2
5Wl3/384 EI
Two constant pressure
Two constant volume
Two isentropic
One constant pressure, one constant volume
Zeroth
First
Second
Third
Zeroth law of thermodynamics
First law of thermodynamics
Second law of thermodynamics
Kelvin Planck's law
For a given compression ratio, both Otto and Diesel cycles have the same efficiency.
For a given compression ratio, Otto cycle is more efficient than Diesel cycle.
For a given compression ratio, Diesel cycle is more efficient than Otto cycle.
The efficiency of Otto or Diesel cycle has nothing to do with compression ratio.
Rankine
Stirling
Carnot
Brayton
11/7
9/7
4/7
All of the above
Isothermally
Isentropically
Polytropically
None of these
wl/6
wl/3
wl
2wl/3
Carnot cycle can't work with saturated steam
Heat is supplied to water at temperature below the maximum temperature of the cycle
A Rankine cycle receives heat at two places
Rankine cycle is hypothetical