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The temperature of a 0.3-L can of soft drink is reduced from 25 to \(6^{\circ} \mathrm{C}\) by a refrigeration cycle. The cycle receives energy by heat transfer from the soft drink and discharges energy by heat transfer at \(25^{\circ} \mathrm{C}\) to the surroundings. There are no other heat transfers. Determine the minimum theoretical work input required, in \(\mathrm{kJ}\), assuming the soft drink is an incompressible liquid with the properties of liquid water. Ignore the aluminum can.

Short Answer

Expert verified
1.626 kJ

Step by step solution

01

Understand the given data and assumptions

The volume of the soft drink is 0.3 L. It cools from 25°C to 6°C. The process is a refrigeration cycle operating between the soft drink and the surroundings at 25°C. The soft drink behaves like liquid water, which is incompressible.
02

Convert units and retrieve properties

The volume of the soft drink is 0.3 L, which is 0.3 kg since 1 L of water has a mass of 1 kg.
03

Determine the heat transfer required

Use the formula \[ Q = m c \triangle T \] where - \( Q \) is the heat removed,- \( m \) is the mass (0.3 kg),- \( c \) is the specific heat capacity of water (4.18 kJ/kg·K),- \( \triangle T \) is the temperature change (25°C - 6°C = 19°C). Substituting the values, we get \[ Q = 0.3 \times 4.18 \times 19 \] \[ Q = 23.874 \text{ kJ} \]
04

Calculate the minimum theoretical work input

Using the Coefficient of Performance (COP) for a refrigeration cycle, \[ \text{COP}_{\text{ref}} = \frac{T_L}{T_H - T_L} \] where \( T_L \) is the lower temperature (279 K) and \( T_H \) is the higher temperature (298 K). Converting the temperatures to Kelvin: \[ T_L = 6 + 273 = 279 \text{ K} \] \[ T_H = 25 + 273 = 298 \text{ K} \] \[ \text{COP} = \frac{279}{298 - 279} = \frac{279}{19} = 14.684 \]
05

Determine the work input

From the relation \[ W = \frac{Q}{\text{COP}} \] where \(Q\) is 23.874 kJ and \( \text{COP} \) is 14.684. Substituting the values, we get \[ W = \frac{23.874}{14.684} = 1.626 \text{ kJ} \]

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Key Concepts

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

thermodynamic cycles
Thermodynamic cycles play a crucial role in refrigeration and many other processes. A thermodynamic cycle involves a series of processes that return a system to its initial state, transferring energy in the form of heat and work. For refrigeration cycles, the primary objective is to move heat from a low-temperature region to a high-temperature region. This process requires work input since heat naturally flows from hot to cold regions. Understanding these cycles helps us optimize energy usage and design more effective refrigeration systems. An example is the cycle used in the problem, where heat is transferred from the soft drink to the surroundings.
heat transfer
Heat transfer is the movement of thermal energy from one object or material to another due to a temperature difference. In the problem, heat transfer occurs when the soft drink cools down. The heat removed from the soft drink is quantified using the formula: \[ Q = mcΔT \]
  • \( Q \) is the amount of heat removed.
  • \( m \) is the mass of the soft drink.
  • \( c \) is the specific heat capacity, which is a property of the material.
  • \( ΔT \) is the temperature change.
In this example, the heat removed from the soft drink is 23.874 kJ, which is then used to calculate the work input for the refrigeration process.
specific heat capacity
Specific heat capacity is the amount of heat required to change the temperature of a unit mass of a substance by one degree. It is a critical property in calculating heat transfer. For water, the specific heat capacity (\( c \)) is 4.18 kJ/kg·K. This value indicates that to change the temperature of 1 kg of water by 1 degree Celsius (or Kelvin), 4.18 kJ of energy is needed. In the given problem, the specific heat capacity of water is used to determine the amount of energy transferred to cool the soft drink from 25°C to 6°C. By knowing the mass (0.3 kg) and the temperature change (19°C), we can apply the formula to calculate the energy removed.
Coefficient of Performance (COP)
The Coefficient of Performance (COP) is a measure of efficiency for refrigeration cycles. It indicates how effectively a refrigeration cycle uses work to transfer heat. The formula for calculating COP in a refrigeration cycle operating between two temperatures is: \[ \text{COP}_{\text{ref}} = \frac{T_L}{T_H - T_L} \] where:
  • \( T_L \) is the lower temperature (in Kelvin).
  • \( T_H \) is the higher temperature (in Kelvin).
The higher the COP, the more efficient the refrigeration cycle. In the problem, the COP is determined to be 14.684, which is then used to calculate the minimum theoretical work input required to cool the soft drink. The formula is: \[ W = \frac{Q}{\text{COP}} \] Using the heat removed (23.874 kJ) and the COP, we find that the minimum theoretical work input is 1.626 kJ.

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Most popular questions from this chapter

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