Heat Q flows spontaneously from a reservoir at 394 K

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In summary, the problem involves spontaneous heat flow from a reservoir at 394 K into a lower temperature reservoir T, resulting in 30% of the heat (Q) being unavailable for work when a Carnot engine operates between these two reservoirs at temperatures T and 248 K. The equation to solve for T is 0.3Q = (T - 248K) * ΔS, where ΔS is the change in entropy of the universe. Once T is solved for, it represents the temperature of the reservoir into which Q is flowing.
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Heat Q flows spontaneously from a reservoir at 394 K into a reservoir that has a lower temerature T. Because of the spontaneous flow, thirty percent of Q is rendered unavailable for work when a Carnot engine operates between the reservoir at temperature T and reservoir at 248 K. Find the temperature T.

First of all... I don't even understand the problem.

I know the change in entropy equals the heat (Q) divided by the temperature (T). I also know that the work unavailable (W) equals the temp of the coldest reservoir multiplied by the change of entropy of the universe.

I would appreciate any help! Thanks
 
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.The temperature T is the temperature of the reservoir into which Q is flowing. The equation you need to solve is: 0.3Q = (T - 248K) * ΔS where ΔS is the change in entropy of the universe due to the flow of heat Q. Once you solve for T, you will have the temperature of the reservoir.
 

1. What is "heat Q"?

"Heat Q" refers to the transfer of thermal energy from one object to another. It is often represented by the symbol Q.

2. What is a "reservoir" in this context?

In this context, a reservoir refers to a large source of thermal energy that is at a constant temperature, meaning it can release or absorb heat without changing its own temperature. An example of a reservoir could be a large body of water or a furnace.

3. Why does heat Q flow spontaneously from a reservoir at 394 K?

This is due to the second law of thermodynamics, which states that heat always flows from hotter objects to colder objects in a natural, irreversible way. Since the reservoir is at a higher temperature of 394 K, heat will naturally flow from it to objects at lower temperatures.

4. Can heat Q flow in the opposite direction?

Yes, it is possible for heat Q to flow in the opposite direction if work is done on the system. For example, if a heat pump is used to transfer heat from a colder area to a warmer area, heat Q will flow in the opposite direction.

5. How is the amount of heat Q calculated in this scenario?

The amount of heat Q transferred can be calculated using the equation Q = mcΔT, where m is the mass of the object, c is its specific heat capacity, and ΔT is the change in temperature. In this scenario, the change in temperature would be the difference between the reservoir temperature of 394 K and the temperature of the object receiving the heat.

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