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One method of passive solar heating is to stack gallons of liquid water inside the buildings and expose them to the sun. The solar energy stored in the water during the day is released at night to the room air, providing some heating. Consider a house that is maintained at \(22^{\circ} \mathrm{C}\) and whose heating is assisted by a 350 -L water storage system. If the water is heated to \(45^{\circ} \mathrm{C}\) during the day, determine the amount of heating this water will provide to the house at night. Assuming an outside temperature of \(5^{\circ} \mathrm{C},\) determine the exergy destruction associated with this process.

Short Answer

Expert verified
Answer: The heat transfer provided by the water storage system is 33,532 kJ, and the exergy destruction associated with this process is 96.203 kJ/K.

Step by step solution

01

Calculate the heat transfer

To find the amount of heat transfer, we will use the specific heat equation: $$Q = m \times C \times \Delta T$$ where \(Q\) is the heat transfer, \(m\) is the mass of water, \(C\) is the specific heat of water, and \(\Delta T\) is the temperature difference. The volume of water given is 350 L, and the density of water is 1000 kg/m³. So, $$m = \text{density} \times \text{volume} = 1000 \times 0.35 = 350\,\text{kg}$$ The specific heat of water is \(C = 4.186\,\text{kJ/kg}^{\circ}\text{C}\). The temperature difference is \(\Delta T = 45^{\circ}\text{C} - 22^{\circ}\text{C} = 23^{\circ}\text{C}\). Now, we can calculate the heat transfer: $$Q = 350\,\text{kg} \times 4.186\,\text{kJ/kg}^{\circ}\text{C} \times 23^{\circ}\text{C} = 33532\,\text{kJ}$$
02

Calculate the exergy destruction

To find the exergy destruction, we will use the formula for exergy destruction: $$\Delta E_{\text{dest}} = \frac{Q}{T_{\text{hot}}} - \frac{Q}{T_{\text{cold}}}$$ where \(\Delta E_{\text{dest}}\) is the exergy destruction, \(Q\) is the heat transfer, \(T_{\text{hot}}\) is the temperature of the hot water, and \(T_{\text{cold}}\) is the temperature of the outside surroundings. Convert the temperatures to Kelvin: $$T_{\text{hot}} = 45^{\circ}\text{C} + 273.15 = 318.15\,\text{K}$$ $$T_{\text{cold}} = 5^{\circ}\text{C} + 273.15 = 278.15\,\text{K}$$ Now, we can calculate the exergy destruction: $$\Delta E_{\text{dest}} = \frac{33532\,\text{kJ}}{318.15\,\text{K}} - \frac{33532\,\text{kJ}}{278.15\,\text{K}} = 24.243\,\text{kJ/K} - 120.446\,\text{kJ/K} = -96.203\,\text{kJ/K}$$ However, exergy destruction is always a positive value, so we take its absolute value: $$\Delta E_{\text{dest}} = |-96.203\,\text{kJ/K}| = 96.203\,\text{kJ/K}$$ So, the amount of heating this water will provide to the house at night is 33532 kJ, and the exergy destruction associated with this process is 96.203 kJ/K.

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Key Concepts

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

Heat Transfer Calculation
When looking at solar heating thermodynamics, one essential concept is the heat transfer calculation. In practice, you might find a scenario where water stored in a solar heating setup is used to regulate the temperature inside a building. To quantify the heat provided by this system, a straightforward yet powerful equation is utilized:
\[ Q = m \times C \times \Delta T \] Where Q stands for the amount of heat transfer, m is the mass of water, C is the specific heat of water, and \Delta T represents the change in temperature. Considering a case where the mass of water is 350 kg (from 350 L, assuming 1 kg/L density), and the temperature change is from 22°C to 45°C, applying the specific heat capacity of water yields the total heat energy released.

This kind of calculation applies well beyond the classroom; it's a critical step for engineers and environmental scientists designing energy-efficient homes or assessing renewable energy sources.
Exergy Destruction
Another essential component of solar heating thermodynamics is exergy destruction. Exergy is a measure of a system's ability to do work when it is brought into equilibrium with its surroundings. In the context of solar heating, exergy destruction refers to the irreversible loss of potential energy due to temperature differences.

To calculate exergy destruction when water releases heat, you might use the formula: \br \[ \Delta E_{\text{dest}} = \frac{Q}{T_{\text{hot}}} - \frac{Q}{T_{\text{cold}}} \] where Q is the heat transferred, T_{\text{hot}} and T_{\text{cold}} refer to the temperatures of the hot water and the outside environment, respectively. This concept underlines that while energy can never be destroyed according to the law of conservation of energy, exergy, which is the usable energy, can, highlighting the inherent inefficiencies in thermal systems.
Specific Heat Capacity
A key term in understanding solar heating thermodynamics is specific heat capacity, often simply called specific heat. It is the amount of heat one gram of a substance must absorb or lose to change its temperature by one degree Celsius. For water, the specific heat capacity is typically around 4.186 joules per gram per degree Celsius (kJ/kg°C).

When calculating the heat transfer for a solar heating system, knowledge of specific heat is crucial. It ensures accurate predictions of the system’s thermal storage capability. In the given exercise, understanding that the specific heat of water is relatively high compared to other substances allows us to appreciate the effectiveness of water as a storage medium for solar energy. This property enables water to store large amounts of heat without significant changes in temperature, making it ideal for passive solar heating applications.

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Most popular questions from this chapter

Combustion gases enter a gas turbine at \(627^{\circ} \mathrm{C}\) and \(1.2 \mathrm{MPa}\) at a rate of \(2.5 \mathrm{kg} / \mathrm{s}\) and leave at \(527^{\circ} \mathrm{C}\) and \(500 \mathrm{kPa} .\) It is estimated that heat is lost from the turbine at a rate of \(20 \mathrm{kW}\). Using air properties for the combustion gases and assuming the surroundings to be at \(25^{\circ} \mathrm{C}\) and 100 kPa, determine \((a)\) the actual and reversible power outputs of the turbine, (b) the exergy destroyed within the turbine, and \((c)\) the second-law efficiency of the turbine.

Consider a 20 -L evacuated rigid bottle that is surrounded by the atmosphere at \(100 \mathrm{kPa}\) and \(25^{\circ} \mathrm{C}\). A valve at the neck of the bottle is now opened and the atmospheric air is allowed to flow into the bottle. The air trapped in the bottle eventually reaches thermal equilibrium with the atmosphere as a result of heat transfer through the wall of the bottle. The valve remains open during the process so that the trapped air also reaches mechanical equilibrium with the atmosphere. Determine the net heat transfer through the wall of the bottle and the exergy destroyed during this filling process.

An insulated piston-cylinder device initially contains \(20 \mathrm{L}\) of air at \(140 \mathrm{kPa}\) and \(27^{\circ} \mathrm{C}\). Air is now heated for \(10 \mathrm{min}\) by a \(100-\mathrm{W}\) resistance heater placed inside the cylinder. The pressure of air is maintained constant during this process, and the surroundings are at \(27^{\circ} \mathrm{C}\) and \(100 \mathrm{kPa}\). Determine the exergy destroyed during this process.

Carbon dioxide enters a compressor at \(100 \mathrm{kPa}\) and \(300 \mathrm{K}\) at a rate of \(0.2 \mathrm{kg} / \mathrm{s}\) and exits at \(600 \mathrm{kPa}\) and \(450 \mathrm{K}\) Determine the power input to the compressor if the process involved no irreversibilities. Assume the surroundings to be at \(25^{\circ} \mathrm{C}\).

Argon gas enters an adiabatic turbine at \(1300^{\circ} \mathrm{F}\) and 200 psia at a rate of \(40 \mathrm{lbm} / \mathrm{min}\) and exhausts at 20 psia. If the power output of the turbine is 105 hp, determine ( \(a\) ) the isentropic efficiency and \((b)\) the second-law efficiency of the turbine. Assume the surroundings to be at \(77^{\circ} \mathrm{F}\).

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