Conservation of work
Conservation of heat
Conversion of heat into work
Conversion of work into heat
C. Conversion of heat into work
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
The amount of heat required to raise the temperature of unit mass of gas through one degree, at constant pressure
The amount of heat required to raise the temperature of unit mass of gas through one degree, at constant volume
The amount of heat required to raise the temperature of 1 kg of water through one degree
Any one of the above
e (1 - 2m)
e (1 - 2/m)
e (m - 2)
e (2/m - 1)
Tensile stress
Compressive stress
Shear stress
Thermal stress
Always in single shear
Always in double shear
Either in single shear or double shear
None of these
Inversely proportional to strain
Directly proportional to strain
Square root of strain
Equal to strain
Otto cycle is more efficient than Diesel cycle
Diesel cycle is more efficient than Otto cycle
Dual cycle is more efficient than Otto and Diesel cycles
Dual cycle is less efficient than Otto and Diesel cycles
Linear stress to linear strain
Linear stress to lateral strain
Volumetric strain to linear strain
Shear stress to shear strain
The shaft 'B' has the greater diameter
The shaft 'A' has the greater diameter
Both are of same diameter
None of these
Sum
Difference
Multiplication
None of the above
(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)
The indirect heat exchanger and cooler is avoided
Direct combustion system is used
A condenser is used
All of the above
Area at the time of fracture
Original cross-sectional area
Average of (A) and (B)
Minimum area after fracture
3/7
7/3
11/3
3/11
In the vertical plane
In the horizontal plane
In the same plane in which the beam bends
At right angle to the plane in which the beam bends
Th > Ts
Th < Ts
Th = Ts
None of these
Acts at a point on a beam
Spreads non-uniformly over the whole length of a beam
Spreads uniformly over the whole length of a beam
Varies uniformly over the whole length of a beam
Two constant volume and two isentropic
Two constant pressure and two isentropic
Two constant volume and two isothermal
One constant pressure, one constant volume and two isentropic
Sum of two principal stresses
Difference of two principal stresses
Half the sum of two principal stresses
Half the difference of two principal stresses
Steel
Copper
Aluminium
None of the above
Zero
Minimum
Maximum
Infinity
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
Unit mass
Modulus of rigidity
Bulk modulus
Modulus of Elasticity
Conservation of heat
Conservation of momentum
Conservation of mass
Conservation of energy
Constant pressure cycle
Constant volume cycle
Constant temperature cycle
Constant temperature and pressure cycle
Swept volume to total volume
Total volume to swept volume
Swept volume to clearance volume
Total volume to clearance volume
Pulverised coal
Brown coal
Coking bituminous coal
Non-coking bituminous coal
11/3 kg of carbon dioxide gas
7/3 kg of carbon monoxide gas
11/7 kg of carbon dioxide gas
8/3 kg of carbon monoxide gas
8/3
11/3
11/7
7/3
Low
Very low
High
Very high