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Question
Consider a heat engine as shown in figure Q1 and Q2 are heat added to heat bath T1 and heat taken from T2 in one cycle of engine. W is the mechanical work done on the engine. If W > 0, then possibilities are ______.
- Q1 > Q2 > 0
- Q2 > Q1 > 0
- Q2 < Q1 < 0
- Q1 < 0, Q2 > 0
Solution
Refrigerator or Heat Pump: A refrigerator or heat pump is basically a heat engine run in the reverse direction. It essentially consists of three parts:
Source: At higher temperatures T1
Working substance: It is called refrigerant liquid ammonia and freon works as a working substance.
Sink: At lower temperature T2. The working substance takes heat Q2 from a sink (contents of the refrigerator) at a lower temperature, has a net amount of work done W on it by an external agent (usual compressor of the refrigerator) and gives out a larger amount of heat Q1, to a hot body at temperature T1 (usually atmosphere). Thus, it transfers heat from a cold body to a hot body at the expense of mechanical energy supplied to it by an external agent. The cold body is thus cooled more and more.
We know that the diagram represents the working of a refrigerator. So, we can write
`Q_1 + W + Q_2`
According to the problem, `W > 0`, then
⇒ `W = Q_1 - Q_2 > 0`
So there are two possibilities:
a. If both `Q_1` and `Q_2` are positive,
⇒ `Q_1 > Q_2 > 0`
c. If both `Q_1` and `Q_2` are positive,
⇒ `Q_2 > Q_1 > 0`
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