0.086
1.086
1.086
4.086
B. 1.086
Tensile
Compressive
Shear
Zero
-273°C
73°C
237°C
-237°C
Maximum calculated value
Minimum calculated value
Mean value
Extreme value
Short column
Long column
Weak column
Medium column
Constant pressure process
Constant volume process
Constant pvn process
All of these
3 to 6
5 to 8
15 to 20
20 to 30
Hookes law
Yield point
Plastic flow
Proof stress
Breaking stress
Fracture stress
Yield point stress
Ultimate tensile stress
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
Wood charcoal
Bituminous coke
Pulverised coal
Coke
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
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.
rγ - 1
1 - rγ - 1
1 - (1/r) γ/γ - 1
1 - (1/r) γ - 1/ γ
Bearing stresses
Fatigue stresses
Crushing stresses
Resultant stresses
Ends are firmly fixed
Column is supported on all sides throughout the length
Length is equal to radius of gyration
Length is twice the radius of gyration
1
1.4
1.67
1.87
2
8
16
32
Temperature limits
Pressure ratio
Volume compression ratio
Cut-off ratio and compression ratio
Same
Twice
Four times
Eight times
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
Creeping
Yielding
Breaking
Plasticity
1/27th
1/93th
1/173th
1/273th
1.817
2512
4.187
None of these
Increases the internal energy of the gas and increases the temperature of the gas
Does some external work during expansion
Both (A) and (B)
None of these
In the middle
At the tip below the load
At the support
Anywhere
The increase in entropy is obtained from a given quantity of heat at a low temperature.
The change in entropy may be regarded as a measure of the rate of the availability or unavailability of heat for transformation into work.
The entropy represents the maximum amount of work obtainable per degree drop in temperature.
All of the above
Greater than
Less than
Equal to
None of these
Becomes constant
Starts decreasing
Increases without any increase in load
None of the above
δl = 4PE/ πl²
δl = 4πld²/PE
δl = 4Pl/πEd₁d₂
δl = 4PlE/ πd₁d₂
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