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By supplying energy to a dwelling at a rate of \(25,000 \mathrm{~kJ} / \mathrm{h}\), a heat pump maintains the temperature of the dwelling at \(20^{\circ} \mathrm{C}\) when the outside air is at \(-10^{\circ} \mathrm{C}\). If electricity costs 8 cents per \(\mathrm{kW} \cdot \mathrm{h}\), determine the minimum theoretical operating cost for each day of operation.

Short Answer

Expert verified
The minimum theoretical operating cost per day is 6 cents.

Step by step solution

01

Understand the problem and given data

The heat pump supplies energy at a rate of 25,000 kJ/h to maintain the temperature of a dwelling at 20°C while the outside temperature is -10°C. Electricity costs 8 cents per kWh. We need to find the minimum theoretical operating cost per day.
02

Convert energy rate to power

First, convert the given energy rate from kJ/h to kW. Power (P) in kW can be calculated as:
03

Determine the Coefficient of Performance (COP) for the heat pump

Calculate the Coefficient of Performance (COP) using the temperature values:
04

Calculate the work input needed

Using the COP, calculate the work input required to deliver the 25,000 kJ/h. Work input (W) can be found by rearranging the COP equation: 0
05

Convert work input to kWh

Convert the work input from kJ/h to kWh:
06

Calculate daily energy consumption

Calculate the energy consumption per day by multiplying the hourly work input by 24 hours: happen corn Lamborghini countyn
07

Determine the cost

Multiply the daily energy consumption by the cost per kWh to find the operating cost per day: car bear lamddit countyn kingnn0

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Key Concepts

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

thermodynamics
Thermodynamics is the branch of physics that deals with the relationships between heat and other forms of energy. It plays a crucial role in understanding how a heat pump operates.

In this exercise, we need to manage the indoor temperature at 20°C when the outdoor temperature is -10°C. This involves transferring heat from a colder environment (outside) to a warmer one (inside).

The principle governing this process is the second law of thermodynamics, which states that heat cannot spontaneously flow from a colder body to a warmer body. A heat pump uses work (energy) to transfer heat uphill against this natural direction.
  • For instance, think of it like a water pump that moves water uphill. Just as moving water requires energy, so does moving heat in thermodynamics.
coefficient of performance
The Coefficient of Performance (COP) is a measure of a heat pump's efficiency. It is defined as the ratio of the heat supplied to the dwelling to the work input. For heating, the COP can be calculated using the formula:
energy conversion
Energy conversion is the process of changing energy from one form to another. In the context of this exercise, we convert electrical energy into thermal energy.



We know that the heat pump supplies energy at a rate of 25,000 kJ/h. To understand how much electrical energy this corresponds to, we need to convert kJ/h to kW (since electricity usage is measured in kilowatt-hours, kWh).
  • To convert, note that 1 kW = 3,600 kJ/h. Hence, 25,000 kJ/h is approximately 6.94 kW.
operating cost calculation
Operating cost calculation helps determine the financial expense of running the heat pump.

After calculating the work input in kWh, we can find the total daily usage by multiplying the hourly energy usage by 24 hours.

Finally, to determine the cost, multiply the daily energy consumption by the cost per kWh. Given that electricity costs 8 cents per kWh:

  • If hourly work input = 6.94 kWh, then daily consumption = 6.94 kWh * 24
  • The daily cost is calculated as: daily consumption * cost per kWh

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Most popular questions from this chapter

A power cycle operates between a reservoir at temperature \(T\) and a lower- temperature reservoir at \(280 \mathrm{~K}\). At steady state, the cycle develops \(40 \mathrm{~kW}\) of power while rejecting 1000 \(\mathrm{kJ} / \mathrm{min}\) of energy by heat transfer to the cold reservoir. Determine the minimum theoretical value for \(T\), in \(\mathrm{K}\).

A refrigeration cycle operating between two reservoirs receives energy \(Q_{\mathrm{C}}\) from a cold reservoir at \(T_{\mathrm{C}}=280 \mathrm{~K}\) and rejects energy \(Q_{\mathrm{H}}\) to a hot reservoir at \(T_{\mathrm{H}}=320 \mathrm{~K}\). For each of the following cases determine whether the cycle operates reversibly, irreversibly, or is impossible: (a) \(Q_{\mathrm{C}}=1500 \mathrm{~kJ}, W_{\text {cycle }}=150 \mathrm{~kJ}\). (b) \(Q_{\mathrm{C}}=1400 \mathrm{~kJ}, Q_{\mathrm{H}}=1600 \mathrm{~kJ}\). (c) \(Q_{\mathrm{H}}=1600 \mathrm{~kJ}, W_{\text {cycle }}=400 \mathrm{~kJ}\). (d) \(\beta=5\).

At steady state, a power cycle having a thermal efficiency of \(38 \%\) generates \(100 \mathrm{MW}\) of electricity while discharging energy by heat transfer to cooling water at an average temperature of \(70^{\circ} \mathrm{F}\). The average temperature of the steam passing through the boiler is \(900^{\circ} \mathrm{F}\). Determine (a) the rate at which energy is discharged to the cooling water, in Btu/h. (b) the minimum theoretical rate at which energy could be discharged to the cooling water, in Btu/h. Compare with the actual rate and discuss.

A hot thermal reservoir is separated from a cold thermal reservoir by a cylindrical rod insulated on its lateral surface. Energy transfer by conduction between the two reservoirs takes place through the rod, which remains at steady state. Using the Kelvin-Planck statement of the second law, demonstrate that such a process is irreversible.

To increase the thermal efficiency of a reversible power cycle operating between reservoirs at \(T_{\mathrm{H}}\) and \(T_{C}\), would you increase \(T_{\mathrm{H}}\) while keeping \(T_{\mathrm{C}}\) constant, or decrease \(T_{\mathrm{C}}\) while keeping \(T_{\mathrm{H}}\) constant? Are there any natural limits on the increase in thermal efficiency that might be achieved by such means?

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