Reversible heat engines use the same working principle as heat engines that include a heat transfer between a cold region and a hot one. However, reverse heat engines also transfer energy in the reverse direction. Instead of transferring energy from a higher temperature region to a lower one, reverse heat engines transfer energy from the colder reservoir to the higher temperature system by adding work.
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Jetzt kostenlos anmeldenReversible heat engines use the same working principle as heat engines that include a heat transfer between a cold region and a hot one. However, reverse heat engines also transfer energy in the reverse direction. Instead of transferring energy from a higher temperature region to a lower one, reverse heat engines transfer energy from the colder reservoir to the higher temperature system by adding work.
Reversible engines work by the principle of the second law of thermodynamics, which states:
Heat transfer naturally occurs only from higher temperature bodies to lower temperature ones but never in the reverse direction. Heat transfer in the reverse direction is only possible with the addition of external work.
A heat engine converts thermal energy from a heat source into mechanical work, while some part of the heat is lost to the surroundings. The work done by a heat engine is defined as the difference between the heat transferred from the hot reservoir and the heat absorbed by the environment, which is at a lower temperature.
The differences between heat and reverse heat engines are listed in the table below.
Reverse heat engines | Heat engines |
Heat is transferred from a cold region to a hot one. | Heat is transferred from a hot region to a colder one. |
Work is added into the system to transfer energy from cold to hot regions (i.e., work is done on the system). | The heat transfer produces work (which is an output from the system). |
Reverse engines convert thermal energy into mechanical work by transferring energy between a hot reservoir and a cold reservoir using a cyclical process. The flow of energy is shown below in figure 1, where the energy is transferred from a lower temperature region to the surroundings (a higher temperature region) by adding work. As this process cannot happen naturally, an electric compressor is used to pump heat out of the system.
\[W + Q_C = Q_H\]
The amount of energy discharged into the surroundings (QH) in Joules by a reverse heat engine is expressed as the sum of the work (W) and the heat transfer from a lower temperature (QC) measured in Joules.
What is the difference between heat and work if they are both measured in Joules?
There are two main reverse heat engine applications: heat pumps and refrigerators, which are designed to remove heat from a cold region and transfer it to a hotter one.
Refrigerators and air conditioners are used to cool down a space by removing heat. Work is done on the system, using a motor to pump warm air inside the fridge to the environment, which is a higher temperature region. The process involves a fluid that is circulated through a closed system:
These steps can be used to construct a p-v diagram, as shown below in figure 2. The amount of heat removed from the fridge per work is given by the coefficient of performance (COPref). It is a measure of the amount of heat transfer from the cold region compared to the work input to the system.
Using the relation between work and heat transfer in a reverse heat engine, we get the following equation for the coefficient of performance:
\[COP_{ref} = \frac{Q_C}{W} = \frac{Q_C}{Q_H-Q_C}\]
For an ideal refrigerator, we assume that the amount of heat transfer in each region is equal to the temperature of the region, which gives us the following expression for COP:
\[COP_{ideal} = \frac{T_C}{T_H-T_C}\]
Power is the work done per unit time measured in Watts or Joules/second
Heat pumps are used to warm up a room. The system is usually comprised of compressed gas, and the sequential working process of a heat pump is as follows:
The amount of heat transferred (QH) into a space per unit work input (W) is the coefficient of performance of a heat pump COPhp.
\[COP_{hp} = \frac{Q_H}{W} = \frac{Q_H}{Q_H-Q_C}\]
\[COP_{ideal} = \frac{T_H}{T_H-T_C}\]
As seen from the equation above, heat pumps seem to have a greater performance when the temperature difference is small. The coefficient of performance is the ratio of heating to required work. Hence, a higher COP means that the heat pump provides the same work with less energy. Therefore, the higher the COP, the higher the efficiency.
The efficiency of a reverse heat engine is the amount of heat transfer that is actually converted into work. This is determined by dividing work by the heat transfer QH. Then, a relation can be written for the COPhp, and the efficiency determined, as seen below.
\[\eta = \frac{W}{Q_H} \text{ or } \eta_{\%} = \frac{W}{Q_H} \cdot 100 \qquad COP_{hp} = \frac{1}{\eta}\]
Since the efficiency of a heat engine is always less than 1 (there will always be some heat lost), COPhp is always greater than 1 (see the equations below). Therefore, a heat pump has more heat transfer Qh than work put into it.
There is also a relation between the refrigerator coefficient of performance and the heat pump coefficient of performance. This can be derived using the equation of work and the heat pump coefficient formula, as seen below.
We begin using the equation that describes the heat transfer in a heat pump:
\[Q_H = Q_C + W\]
Then, we use the heat pump coefficient of performance and refrigerator coefficient of performance equations and re-arrange them in terms of QH and QC, respectively:
\[COP_{hp} = \frac{Q_H}{W} \Rightarrow Q_H = COP_{hp} \cdot W\]
\[COP_{ref} = \frac{Q_C}{W} \Rightarrow Q_C = COP_{ref} \cdot W\]
We now substitute them into the heat transfer equation mentioned earlier and divide by the work on both sides of the equation, which gives us:
\[COP_{hp} \cdot W = COP_{ref} \cdot W +W \qquad \frac{COP_{hp} \cdot W}{W} = \frac{COP_{ref} \cdot W}{W} + \frac{W}{W}COP_{hp} = COP_{ref} + 1 \text { or } COP_{ref} = COP_{hp}-1\]
A refrigerator has a COP of 4.8 and uses 400 J of work. Determine the heat transferred and the efficiency of the refrigerator.
We use the COP formula and substitute the value of the coefficient of performance and work to find the heat transferred.
\(COP_{ref} = \frac{Q_C}{W} \Rightarrow Q_C = COP_{ref} \cdot W = 4.8 \cdot 400 \qquad Q_C = 1920 J\)
To determine the efficiency, we need to find QH. Hence, we need to use the heat transferred and the work to calculate it. Then, we can use the efficiency formula to calculate efficiency, using heat lost QH and work.
\(Q_H = Q_C + W = 1920 + 400 = 2320 J \quad \eta = \frac{W}{Q_H} = \frac{400}{2320} = 0.1724 \quad n_{\%} = 0.1724 \cdot 100 = 17.24\%\)
It is an engine that does work by transferring energy from a lower temperature body to a higher temperature body.
In a heat engine, heat is transferred from hot reservoir to a colder one, whereas in a reverse heat engine, heat is transferred from a colder to a hotter region.
Yes, reversible heat engines are possible by providing additional external work.
A reversible heat engine is an engine that transfer heat from a lower temperature object to a higher temperature object by adding external work, usually using electric motors.
The efficiency of a reverse heat engine is found by the dividing the work by the heat transfer as shown below.
η= W/ QH
What is a reversible heat engine?
It is a heat engine that transfers energy in the reverse direction, i.e., from a lower to a higher temperature region, with the use of additional work.
What is the working principle of a reverse engine?
The second law of thermodynamics states that a heat transfer occurs naturally only from higher temperature bodies to lower temperature ones but never in the reverse direction. A reverse direction transfer is only possible with the addition of external work.
What are the main differences between heat and reverse heat engines in terms of the heat transfer?
In a heat engine, heat is transferred from a hotter to a colder reservoir, whereas in a reverse heat engine, it is transferred from a colder to a hotter region.
What are the differences between heat engines and reverse heat engines in terms of work?
In a heat engine, the heat transfer produces work, while in a reverse heat engine, work is input into the system for the heat transfer.
What is the direction of heat transfer and work in a reverse heat engine?
The energy is transferred from a lower temperature region to the surroundings, which is at a higher temperature region, by adding work.
Why are both heat and work measured in Joules?
They are both forms of energy but have a different characteristic with regard to their motion: heat is a disordered motion of atoms, while work is an ordered motion of atoms in one direction.
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