1.013 bar
760 mm of Hg
1013 × 102 N/m2
All of these
D. All of these
1 N-m/s
100 N-m
1000 N-m/s
1 × 106 N-m/s
Lap joint
Butt joint
Single riveted single cover butt joint
Double riveted double cover butt joint
The indirect heat exchanger and cooler is avoided
Direct combustion system is used
A condenser is used
All of the above
Bearing stresses
Fatigue stresses
Crushing stresses
Resultant stresses
Increase
Decrease
Remain unchanged
Increase/decrease depending on application
Volumetric stress and volumetric strain
Lateral stress and lateral strain
Longitudinal stress and longitudinal strain
Shear stress to shear strain
Rubber
Plastic
Brass
Steel
Kh > Ks
Kh < Ks
Kh = Ks
None of these
2.1 × 10⁵ kg/cm²
2.1 × 10⁶ kg/cm²
2.1 × 10⁷ kg/cm²
0.1 × 10⁶ kg/cm²
Sum of two principal stresses
Difference of two principal stresses
Half the sum of two principal stresses
Half the difference of two principal stresses
Bending moment (i.e. M)
Bending moment² (i.e. M²)
Bending moment³ (i.e. M³)
Bending moment⁴ (i.e. M⁴)
9/7
11/7
7/4
1/4
Load/original cross-sectional area and change in length/original length
Load/ instantaneous cross-sectional area and loge (original area/ instantaneous area)
Load/ instantaneous cross-sectional area and change in length/ original length
Load/ instantaneous area and instantaneous area/original area
Steel
Copper
Aluminium
None of the above
Equal to
Less than
Greater than
None of these
Linear stress to lateral strain
Lateral strain to linear strain
Linear stress to linear strain
Shear stress to shear strain
Plastic limit
Elastic limit
Yield point
Limit of proportionality
More than 50 %
25-50 %
10-25 %
Negligible
Wood charcoal
Bituminous coke
Pulverised coal
Coke
Same
More
Less
Unpredictable
Working substance
Design of engine
Size of engine
Temperatures of source and sink
δl = 4PE/ πl²
δl = 4πld²/PE
δl = 4Pl/πEd₁d₂
δl = 4PlE/ πd₁d₂
Pitch
Back pitch
Diagonal pitch
Diametric pitch
Maximum calculated value
Minimum calculated value
Mean value
Extreme value
Constant volume process
Adiabatic process
Constant pressure process
Isothermal process
Workdone
Entropy
Enthalpy
None of these
In tension
In compression
Neither in tension nor in compression
None of these
(T1/T2) - 1
1 - (T1/T2)
1 - (T2/T1)
1 + (T2/T1)
Zero
Minimum
Maximum
Positive
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