Yield point
Limit of proportionality
Breaking point
Elastic limit
B. Limit of proportionality
Same
Half
Two times
Four times
Pulverised coal
Brown coal
Coking bituminous coal
Non-coking bituminous coal
(Net work output)/(Workdone by the turbine)
(Net work output)/(Heat supplied)
(Actual temperature drop)/(Isentropic temperature drop)
(Isentropic increase in temperature)/(Actual increase in temperature)
Sum of two specific heats
Difference of two specific heats
Product of two specific heats
Ratio of two specific heats
Boyle's law
Charles' law
Gay-Lussac law
Avogadro's law
Greater than
Less than
Equal to
None of these
Oxygen
Sulphur
Nitrogen
Carbon
Principal stresses
Normal stresses on planes at 45°
Shear stresses on planes at 45°
Normal and shear stresses on a plane
Dual combustion cycle
Diesel cycle
Atkinson cycle
Rankine cycle
pv = C
pv = m R T
pvn = C
pvγ = C
Equal to
Half
Double
Quadruple
Change the shape of the beam
Effect the saving in material
Equalise the strength in tension and compression
Increase the cross-section of the beam
400 MPa
500 MPa
900 MPa
1400 MPa
Greater than
Less than
Equal to
None of these
v1/v2
v2/v1
(v1 + v2)/v1
(v1 + v2)/v2
Increasing the internal energy of gas
Doing some external work
Increasing the internal energy of gas and also for doing some external work
None of the above
Hookes law
Yield point
Plastic flow
Proof stress
Joint less section
Homogeneous section
Perfect section
Seamless section
Not deform
Be safest
Stretch
Not stretch
Zeroth law of thermodynamics
First law of thermodynamics
Second law of thermodynamics
None of these
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
rγ - 1
1 - rγ - 1
1 - (1/r) γ/γ - 1
1 - (1/r) γ - 1/ γ
The pressure and temperature of the working substance must not differ, appreciably, from those of the surroundings at any stage in the process
All the processes, taking place in the cycle of operation, must be extremely slow
The working parts of the engine must be friction free
All of the above
Volumetric stress and volumetric strain
Lateral stress and lateral strain
Longitudinal stress and longitudinal strain
Shear stress to shear strain
Two isothermal and two isentropic
Two isentropic and two constant volumes
Two isentropic, one constant volume and one constant pressure
Two isentropic and two constant pressures
Doubled
Halved
Becomes four times
None of the above
All the reversible engines have the same efficiency.
All the reversible and irreversible engines have the same efficiency.
Irreversible engines have maximum efficiency.
All engines are designed as reversible in order to obtain maximum efficiency.
Its length is very small
Its cross-sectional area is small
The ratio of its length to the least radius of gyration is less than 80
The ratio of its length to the least radius of gyration is more than 80
Wl3/48 EI
Wa²b²/3EIl
[Wa/(a√3) x EIl] x (l² - a²)3/2
5Wl3/384 EI
Increase key length
Increase key depth
Increase key width
Double all the dimensions