Suction pressure
Discharge pressure
Critical pressure
Back pressure
B. Discharge pressure
1 + C.O.P
1 - C.O.P.
1 + (1/C.O.P)
1 - (1/C.O.P)
Less than 2 kg
More than or equal to 3.65 kg
More than 10 kg
There is no such consideration
Reciprocating
Rotating
Centrifugal
Screw
Heat supplied by the gas burner to the heat absorbed by the evaporator
Heat absorbed by the evaporator to the heat supplied by the gas burner
Heat supplied by the gas burner minus the heat absorbed by the evaporator to the heat supplied by the gas burner
Heat absorbed by the evaporator minus the heat supplied by the gas burner to the heat absorbed by the evaporator
Ammonia
Carbon dioxide
Sulphur dioxide
R-12
In 1 hour
In 1 minute
In 24 hours
In 12 hours
0.1 ton
5 tons
10 tons
40 tons
Does not alter C.O.P.
Increases C.O.P.
Decreases C.O.P.
None of these
Same as
Lower than
Higher than
None of these
3.5/C.O.P.
C.O.P/3.5
3.5 × C.O.P.
None of these
The performance of the vapour compression refrigerator varies considerably with both vaporising and condensing temperatures.
In vapour compression cycle, the useful part of the heat transfer is at the condenser.
In ammonia-hydrogen (Electrolux) refrigerator, no compressor, pump or fan is required.
The effect of under-cooling the liquid refrigerant is to decrease the coefficient of performance.
(C.O.P.)P = (C.O.P.)R + 2
(C.O.P.)P = (C.O.P.)R + 1
(C.O.P)P = (C.O.P)R - 1
(C.O.P)P = (C.O.P)R
(Theoretical C.O.P.)/ (Actual C.O.P.)
(Actual C.O.P.) /(Theoretical C.O.P.)
(Actual C.O.P.) × (Theoretical C.O.P.)
None of these
Iron
Lead
Aluminium
Rubber
Ammonia
R-12
Sulphur dioxide
Carbon dioxide
System has high C.O.P.
Power per TR is low
Mass of refrigerant circulated in the system is low
Mass of the refrigeration equipment is low
Suction pressure
Discharge pressure
Critical pressure
Back pressure
High pressure saturated liquid
Wet vapour
Very wet vapour
Dry vapour
Low weight per tonne of refrigeration
High heat transfer rate
Low temperature at high altitudes
Higher coefficient of performance
Pressure lines
Temperature lines
Total heat lines
Entropy lines
Noisy operation
Quiet operation
Cooling below 0°C
Very little power consumption
25 kJ/kg
50 kJ/kg
100 kJ/kg
125 kJ/kg
Above which liquid will remain liquid
Above which liquid becomes gas
Above which liquid becomes vapour
Above which liquid becomes solid
Equalise
Reduce
Increase
None of these
Same
Lower
Higher
None of these
NN = hl/k
NN = μ cp/k
NN = ρ V l /μ
NN = V²/t.cp
Electrically operated throttling valve
Manually operated valve
Thermostatic valve
Capillary tube
Wet vapour region
Superheated vapour region
Sub-cooled liquid region
None of these
The human body can lose heat even if its temperature is less than the atmospheric temperature.
The increase in air movement increases the evaporation from the human body.
The warm air increases the rate of radiation of heat from the human body.
Both (A) and (B)
It is not affected by the moisture present in the air
Its bulb is surrounded by a wet cloth exposed to the air
The moisture present in it begins to condense
None of the above