The heat and work are boundary phenomena
The heat and work represent the energy crossing the boundary of the system
The heat and work are path functions
All of the above
D. All of the above
Dual cycle, Diesel cycle, Otto cycle
Otto cycle, Diesel cycle, Dual cycle
Dual cycle, Otto cycle, Diesel cycle
Diesel cycle, Otto cycle, Dual cycle
Wood charcoal
Bituminous coal
Briquetted coal
None of these
Simply supported beam
Fixed beam
Overhanging beam
Cantilever beam
Greater than
Less than
Equal to
None of these
Increase
Decrease
Remain unchanged
Increase/decrease depending on application
Unit mass
Modulus of rigidity
Bulk modulus
Modulus of Elasticity
Sum of two specific heats
Difference of two specific heats
Product of two specific heats
Ratio of two specific heats
Carbon and hydrogen
Oxygen and hydrogen
Sulphur and oxygen
Sulphur and hydrogen
-100 MPa
250 MPa
300 MPa
400 MPa
Carbon
Hydrogen and nitrogen
Sulphur and ash
All of these
Equal to
Less than
Greater than
None of these
Isothermal
Isentropic
Polytropic
None of these
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
237°C
-273°C
-237°C
273°C
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.
1
0
-1
10
cv/ cp =R
cp - cv = R
cv = R/ γ-1
Both (B) and (C)
Pressure exerted by the gas
Volume occupied by the gas
Temperature of the gas
All of these
Resilience
Proof resilience
Strain energy
Impact energy
Very low
Low
High
Very high
Positive
Negative
Positive or negative
None of these
Greater than
Less than
Equal to
None of these
Resilience
Proof resilience
Modulus of resilience
Toughness
Temperature limits
Pressure ratio
Compression ratio
Cut-off ratio and compression ratio
Same
Twice
Four times
Eight times
δl = 4PE/ πl²
δl = 4πld²/PE
δl = 4Pl/πEd₁d₂
δl = 4PlE/ πd₁d₂
Reversible cycles
Irreversible cycles
Semi-reversible cycles
Adiabatic irreversible cycles
Brayton cycle
Joule cycle
Carnot cycle
Reversed Brayton cycle
It is impossible to construct an engine working on a cyclic process, whose sole purpose is to convert heat energy into work
It is possible to construct an engine working on a cyclic process, whose sole purpose is to convert heat energy into work
It is impossible to construct a device which operates in a cyclic process and produces no effect other than the transfer of heat from a cold body to a hot body
None of the above
Isothermal process
Adiabatic process
Free expansion process
Throttling process