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A nuclear power plant has an electrical power output of \(1000 \mathrm{MW}\) and operates with an efficiency of \(39 \%\). If excess energy is carried away from the plant by a river with a flow rate of \(1.0 \times 10^{6} \mathrm{~kg} / \mathrm{s}\), what is the rise in temperature of the flowing water?

Short Answer

Expert verified
The rise in temperature of the flowing water is approximately \(0.37 K\).

Step by step solution

01

Calculate the total power produced by the plant

Using the efficiency formula \( \text{Efficiency} = \frac{\text{Useful Power}}{\text{Total Power}} \), we can find the total power produced by rearranging the formula to \( \text{Total Power} = \frac{\text{Useful Power}}{\text{Efficiency}} \). Substituting the given values, \( \text{Total Power} = \frac{1000MW}{0.39} = 2564.10 MW \)
02

Find the wasted power

The wasted power can be found by subtracting the useful power from the total power. \( \text{Wasted Power} = \text{Total Power} - \text{Useful Power} = 2564.10 MW - 1000 MW = 1564.10 MW \). However, it is important to convert this power to watt by multiplying it by \(10^6\) to facilitate further calculations, so the wasted power becomes \(1564.10 \times 10^6 W\)
03

Calculate the rise in temperature

By using the formula for heat transfer \( Q = mc \Delta T \), where \( Q \) is the heat energy, \( m \) is the mass, \( c \) is the specific heat capacity of water (\(4.18 \times 10^3 J/kgK\)), and \( \Delta T \) is the change in temperature, we can isolate \( \Delta T \) from this formula to get \( \Delta T = \frac{Q}{mc} \). Substituting \( Q \) with the wasted power and using the values for \( m \) and \( c \), we get \( \Delta T = \frac{1564.10 \times 10^6 W}{1.0 \times 10^6 kg/s \times 4.18 \times 10^3 J/kgK} = 0.37 K \)

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Nuclear Power Plant Efficiency
Nuclear power plants generate electricity by harnessing the energy released from nuclear reactions. Efficiency in this context refers to how well the plant converts nuclear energy into electrical energy. It is calculated by dividing the useful (electrical) power output by the total power produced. In the given exercise, the power plant has an efficiency of 39%. This means that for every 100 units of energy produced, only 39 units are converted into usable electrical energy, while the remaining 61 units are lost as waste heat.

To find the total energy produced, you can rearrange the efficiency formula:
  • Efficiency (\( \eta \text{) = } \frac{\text{Useful Power} (P_{\text{useful}})}{\text{Total Power} (P_{\text{total}})} \)
  • Rearranged, it becomes: \( P_{\text{total}} = \frac{P_{\text{useful}}}{\eta} \).
  • Substituting given values: \( P_{\text{total}} = \frac{1000 \text{ MW}}{0.39} = 2564.10 \text{ MW} \).
Understanding efficiency helps in optimizing operations and reducing unnecessary energy losses. By enhancing efficiency, plants can produce more electricity with the same amount of nuclear material.
Heat Transfer
Heat transfer is a key principle in thermodynamics and plays an essential role in nuclear power plant operations. In this exercise, the excess energy not converted into electricity is carried away by water from a nearby river. This process of heat removal is crucial to prevent overheating.

Heat transfer in this context can be quantified using the formula:
  • \( Q = mc \Delta T \)
  • Here, \( Q \) is the heat energy (in Joules), \( m \) is the mass flow rate of the water (in kg/s), \( c \) is the specific heat capacity of the medium (water, in this case), and \( \Delta T \) is the change in temperature (in Kelvin or Celsius).
By rearranging the formula to solve for the temperature change, you can determine how much the water's temperature rises as it absorbs the excess energy:
  • \( \Delta T = \frac{Q}{mc} \).
Accurate calculations of heat transfer ensure that waste heat is managed effectively, maintaining safe and efficient plant operations.
Specific Heat Capacity
Specific heat capacity is a vital concept in the study of thermodynamics. It refers to the amount of heat required to change the temperature of a unit mass of a substance by one degree Celsius. For water, which often plays a fundamental role in power generation, the specific heat capacity is approximately \(4.18 \times 10^3 \text{ J/kgK} \).

Understanding water's specific heat capacity is essential in evaluating its effectiveness as a cooling agent in nuclear power plants. Water is chosen frequently due to its high specific heat capacity, allowing it to absorb substantial amounts of heat with only a slight increase in temperature. This property of water helps in:
  • Efficiently capturing large amounts of waste heat
  • Minimizing the risks associated with overheating
  • Maintaining regular operational temperatures.
In the exercise, the specific heat capacity of water facilitates the calculation of the temperature rise \( \Delta T \), providing insight into the cooling process's efficiency. The ability to absorb significant amounts of heat makes water an indispensable part of thermodynamic systems in nuclear power plants.

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Most popular questions from this chapter

A freezer has a coefficient of performance of \(6.30\). The freezer is advertised as using \(457 \mathrm{~kW}-\mathrm{h} / \mathrm{y}\). (a) On average, how much energy does the freezer use in a single day? (b) On average, how much thermal energy is removed from the freezer each day? (c) What maximum amount of water at \(20.0^{\circ} \mathrm{C}\) could the freezer freeze in a single day? (One kilowatt-hour is an amount of energy equal to running a \(1-\mathrm{kW}\) appliance for one hour.)

Sketch a PV diagram of the following processes: (a) A gas expands at constant pressure \(P_{1}\) from volume \(V_{1}\) to volume \(V_{2} .\) It is then kept at constant volume while the pressure is reduced to \(P_{2}\). (b) A gas is reduced in pressure from \(P_{1}\) to \(P_{2}\) while its volume is held constant at \(V_{1} .\) It \(i s\) then expanded at constant pressure \(P_{2}\) to a final volume \(V_{2} .(c)\) In which of the processes is more work done by the gas? Why?

A gas changes in volume from \(0.750 \mathrm{~m}^{3}\) to \(0.250 \mathrm{~m}^{3}\) at a constant pressure of \(1.50 \times 10^{\circ}\) Pa. (a) How much work is done on the gas? (b) How much work is done by the gas on its environment? (c) Which of Newton's laws best explains why the work done on the gas is the negative of the work done on the environment?

A power plant has been proposed that would make use of the temperature gradient in the ocean. The system is to operate between \(20.0^{\circ} \mathrm{C}\) (surface water temperature) and \(5.00^{\circ} \mathrm{C}\) (water temperature at a depth of about \(1 \mathrm{~km}\). (a) What is the maximum efficiency of such a system? (b) If the useful power output of the plant is \(75.0 \mathrm{MW}\), how much energy is absorbed per hour? (c) In view of your answer to part (a), do you think such a system is worthwhile (considering that there is no charge for fuel)?

The only form of energy possessed by molecules of a monatomic ideal gas is translational kinetic energy. Using the results from the discussion of kinetic theory in SecLion \(10.5\), show that the internal energy of a monatomic ideal gas at pressure \(P\) and occupying volume \(V\) may be written as \(U=\frac{3}{2} P V\)

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