Thermodynamics Heat Engine Problem

In summary, a power plant delivering energy at 918MW using superheated steam turbines with a temperature of 626K and deposits its unused heat in river water at 286K. Assuming it operates as an ideal Carnot engine, with a river flow rate of 40.4m^3/s, the average temperature increase of the river water downstream from the power plant is 2.5 degrees Celsius. The entropy increase per kilogram of the downstream river water can be calculated using the equations: (Q_H)/(T_H)=(Q_L)/(T_L), delta(Q)=(m)(c)(delta(T)), and delta(S)=(m)(c)ln((T_F)/(T_I)).
  • #1
smithnh
11
0
Thank you in advance...

1. Homework Statement

Suppose a power plant delivers energy at 918MW using steam turbines. The steam goes into the turbines superheated at 626K and deposits its unused heat in river water at 286K. Assume that the turbine operates as an ideal Carnot engine. If the river flow rate is 40.4m^3/s, calculate the average temperature increase (in Celsius) of the river water downstream from the power plant. What is the entropy increase per kilogram of the downstream river water?


2. Homework Equations

(Q_H)/(T_H)=(Q_L)/(T_L)

delta(Q)=(m)(c)(delta(T))

delta(S)=(m)(c)ln((T_F)/(T_I))


3. The Attempt at a Solution

(918 MW)/(626K)=(Q_L)/(286K) so Q_L= 419.4 MW

(419400000 J/s)= (40.3 m^3/s)*(10^6 g/m^3)*(4.186 J/g/K)*delta(T)

so delta(T)= 2.5 celcius degrees right?
 
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  • #2
smithnh said:
Thank you in advance...

1. Homework Statement

Suppose a power plant delivers energy at 918MW using steam turbines. The steam goes into the turbines superheated at 626K and deposits its unused heat in river water at 286K. Assume that the turbine operates as an ideal Carnot engine. If the river flow rate is 40.4m^3/s, calculate the average temperature increase (in Celsius) of the river water downstream from the power plant. What is the entropy increase per kilogram of the downstream river water?2. Homework Equations

(Q_H)/(T_H)=(Q_L)/(T_L)

delta(Q)=(m)(c)(delta(T))

delta(S)=(m)(c)ln((T_F)/(T_I))

[tex]\eta = \frac{W}{\Delta Q_h} [/tex] so

[tex]\Delta Q_h = \frac{W}{\eta}[/tex]

Work out the efficiency from the temperature difference. Then determine the work/unit time from the output power. That will tell you the heat per unit time ([itex]dQ_h/dt[/tex]) delivered from the hot reservoir. You then work out what the heat flow to the cold reservoir is per unit time. Then work out the increase in temperature of the river water and the entropy change in the cold reservoir / unit mass using [tex]\Delta S = \Delta Q/T[/tex]

AM
 
  • #3


delta(S)=(40.3 m^3/s)*(10^6 g/m^3)*(4.186 J/g/K)*ln((288.5K)/(286K)) = 1.71 J/K

I would like to first clarify that the calculations done in the attempt at a solution are correct. The Carnot efficiency formula (Q_H/T_H = Q_L/T_L) and the heat transfer equation (Q = mc∆T) were appropriately used to determine the temperature increase of the river water downstream from the power plant and the entropy increase per kilogram of the downstream river water.

However, it is important to note that the assumptions made in this problem, such as the ideal Carnot engine and the constant river flow rate, may not accurately reflect real-world situations. In reality, power plants may not operate at ideal efficiency and river flow rates can vary.

Furthermore, the increase in temperature and entropy of the river water can have potential impacts on the surrounding ecosystem. As a scientist, it is important to consider the potential consequences of energy production on the environment and work towards finding sustainable and efficient solutions.

In conclusion, while the calculations done in this problem provide a theoretical answer, it is crucial to consider the practical implications and limitations of such a scenario in the real world.
 

1. What is a heat engine?

A heat engine is a device that converts thermal energy into mechanical energy. It operates by taking in heat from a high-temperature source, using it to do work, and then releasing the remaining heat to a low-temperature sink.

2. What is the first law of thermodynamics?

The first law of thermodynamics is also known as the law of conservation of energy. It states that energy cannot be created or destroyed, only transformed from one form to another. In the context of a heat engine problem, this means that the total energy entering the system (heat) must equal the total energy leaving the system (work done + remaining heat).

3. What is the second law of thermodynamics?

The second law of thermodynamics states that the total entropy (measure of disorder) of a closed system will always increase over time. In the context of a heat engine problem, this means that not all of the heat energy can be converted into work, and some will always be lost to the environment.

4. How do you calculate the efficiency of a heat engine?

The efficiency of a heat engine is calculated by dividing the work output by the heat input. Mathematically, it can be represented as: efficiency = work output / heat input. It is always less than 1 (or 100%) due to the second law of thermodynamics.

5. How does the Carnot cycle relate to heat engine problems?

The Carnot cycle is a theoretical cycle that represents the most efficient way to convert heat energy into work. It consists of four processes: isothermal expansion, adiabatic expansion, isothermal compression, and adiabatic compression. Although no real heat engine can achieve Carnot efficiency, it serves as a useful benchmark for comparing the efficiency of real heat engines.

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