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For each \(\mathrm{kW}\) of power input to an ice maker at steady state, determine the maximum rate that ice can be produced, in \(\mathrm{kg} / \mathrm{h}\), from liquid water at \(0^{\circ} \mathrm{C}\). Assume that \(333 \mathrm{~kJ} / \mathrm{kg}\) of energy must be removed by heat transfer to freeze water at \(0^{\circ} \mathrm{C}\), and that the surroundings are at \(20^{\circ} \mathrm{C}\).

Short Answer

Expert verified
10.81 kg/h

Step by step solution

01

- Identify given values

The power input to the ice maker is 1 kW. The latent heat of fusion for water is given as 333 kJ/kg. The surroundings are at 20°C and the freezing point of water is 0°C.
02

- Understand the problem

We need to find the maximum rate of ice production in kg/h from liquid water at 0°C with a given power input of 1 kW, while assuming that 333 kJ/kg of energy must be removed to freeze the water.
03

- Calculate the energy input per hour

First, convert the power input from kW to kJ/h. Since 1 kW = 1 kJ/s, multiply by the number of seconds in an hour (3600 s). 1 kW = 1 kJ/s Energy input per hour = 1 kW * 3600 s = 3600 kJ/h.
04

- Calculate the mass of ice produced

Using the given latent heat of fusion for water, calculate how much ice can be produced by the energy input. Energy required to freeze 1 kg of water = 333 kJ Maximum mass of ice produced per hour = Energy input per hour / Latent heat of fusion Therefore, mass of ice = 3600 kJ/h / 333 kJ/kg = 10.81 kg/h.

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Key Concepts

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

Latent Heat of Fusion
The latent heat of fusion is the amount of energy required to change a substance from the solid phase to the liquid phase without changing its temperature. In our exercise, we deal with freezing water, so we are focusing on the inverse process.
For water, the latent heat of fusion is given as 333 kJ/kg. This means that 333 kJ of energy must be removed from 1 kg of liquid water at 0°C to convert it to ice at 0°C. This energy removal happens without a change in temperature, just like the heat added does not change the temperature during melting.
This concept is crucial in ice-making processes. By removing 333 kJ of energy per kg of water, we are able to convert it into ice. Understanding this helps in calculating the efficiency and effectiveness of thermal systems like ice makers.
Energy Conversion
Energy conversion is the process of changing energy from one form to another. In our example exercise, the ice maker converts electrical energy into thermal energy to remove heat from water, thus freezing it.
The power input we considered is 1 kW, equivalent to 1 kJ/s. To find out how much energy is applied over an hour, we multiply the power by the number of seconds in an hour (3600 seconds), yielding 3600 kJ/h.
This energy conversion process is vital in various household and industrial applications. Each application, like water freezing, requires a specific amount of energy conversion, based on the substance's physical properties, such as the latent heat of fusion.
Having a good grasp of these conversion principles allows efficient design and operation of thermal systems.
Steady State Processes
In thermodynamics, a steady state process is a condition where all state variables remain constant despite ongoing processes. In this context, our ice maker operates at a steady state, meaning the rate at which energy is added equals the rate at which energy is removed.
Because the ice maker is in steady state, the power input is consistently being converted to thermal energy to remove heat from water. This consistent removal of energy ensures that the rate of ice production remains constant.
Calculations in steady state make theoretical analysis simpler because we do not account for changes over time—everything is considered in equilibrium.
This allows the determination of maximum rates of processes, like ice production, under specified conditions. Understanding steady state helps in predicting the performance and efficiency of devices and systems across various applications.

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Most popular questions from this chapter

A building for which the heat transfer rate through the walls and roof is \(400 \mathrm{~W}\) per degree temperature difference between the inside and outside is to be maintained at \(20^{\circ} \mathrm{C}\). For a day when the outside temperature is \(4^{\circ} \mathrm{C}\), determine the power required at steady state, \(\mathrm{kW}\), to heat the building using electrical resistance elements and compare with the minimum theoretical power that would be required by a heat pump. Repeat the comparison using typical manufacturer's data for the heat pump coefficient of performance.

Using the Kelvin-Planck statement of the second law of thermodynamics, demonstrate the following corollaries: (a) The coefficient of performance of an irreversible refrigeration cycle is always less than the coefficient of performance of a reversible refrigeration cycle when both exchange energy by heat transfer with the same two reservoirs. (b) All reversible refrigeration cycles operating between the same two reservoirs have the same coefficient of performance. (c) The coefficient of performance of an irreversible heat pump cycle is always less than the coefficient of performance of a reversible heat pump cycle when both exchange energy by heat transfer with the same two reservoirs. (d) All reversible heat pump cycles operating between the same two reservoirs have the same coefficient of performance.

Abandoned lead mines near Park Hills, Missouri are filled with an estimated \(2.5 \times 10^{8} \mathrm{~m}^{3}\) of water at an almost constant temperature of \(14^{\circ} \mathrm{C}\). How might this resource be exploited for heating and cooling of the town's dwellings and commercial buildings? A newspaper article refers to the water-filled mines as a free source of heating and cooling. Discuss this characterization.

Two kilograms of water execute a Camot power cycle. During the isothermal expansion, the water is heated until it is a saturated vapor from an initial state where the pressure is 40 bar and the quality is \(15 \%\). The vapor then expands adiabatically to a pressure of \(1.5\) bar while doing \(491.5 \mathrm{~kJ} / \mathrm{kg}\) of work. (a) Sketch the cycle on \(p-v\) coordinates. (b) Evaluate the heat and work for each process, in \(\mathrm{kJ}\). (c) Evaluate the thermal efficiency.

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 \(\mathrm{K}\).

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