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In a dairy operation, milk at a flow rate of \(250 \mathrm{~L} / \mathrm{h}\) and a cow-body temperature of \(38.6^{\circ} \mathrm{C}\) must be chilled to a safe-to-store temperature of \(13^{\circ} \mathrm{C}\) or less. Ground water at \(10^{\circ} \mathrm{C}\) is available at a flow rate of \(0.72 \mathrm{~m}^{3} / \mathrm{h}\). The density and specific heat of milk are \(1030 \mathrm{~kg} / \mathrm{m}^{3}\) and \(3860 \mathrm{~J} / \mathrm{kg} \cdot \mathrm{K}\), respectively. (a) Determine the UA product of a counterflow heat exchanger required for the chilling process. Determine the length of the exchanger if the inner pipe has a 50 -mm diameter and the overall heat transfer coefficient is \(U=1000 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\). (b) Determine the outlet temperature of the water. (c) Using the value of \(U A\) found in part (a), determine the milk outlet temperature if the water flow rate is doubled. What is the outlet temperature if the flow rate is halved?

Short Answer

Expert verified
In a counterflow heat exchanger for chilling milk, with given conditions, we determined that: 1. The UA product required for the chilling process is 110037.3 W/K, and the length of the exchanger with a 50-mm inner pipe diameter is 7.013 meters. 2. The outlet temperature of the ground water is 26.5°C. 3. If the water flow rate is doubled, the milk outlet temperature is 13.97°C, and if the water flow rate is halved, the milk outlet temperature is 16.96°C.

Step by step solution

01

Part A - Determine the UA product and Length of the Exchanger

First, we need to calculate the mass flow rate and heat capacity rate of milk using its properties and flow rate: 1. Convert the milk flow rate from L/h to m³/h: \( 250 L/h = \frac{250}{1000} m^3/h = 0.25 m^3/h \) 2. Calculate the mass flow rate of milk: \( \dot{m}_{milk} = \rho_{milk} \times \dot{V}_{milk} = 1030 kg/m^3 \times 0.25 m^3/h = 257.5 kg/h \) 3. Calculate the heat capacity rate of milk: \( C_{milk} = \dot{m}_{milk} \times c_{p,milk} = 257.5 kg/h \times 3860 J/kgK = 994025 J/hK \) Now let's calculate the mass flow rate and heat capacity rate of the ground water: 1. Calculate the mass flow rate of water: \( \dot{m}_{water} = \rho_{water} \times \dot{V}_{water} = 1000 kg/m^3 \times 0.72 m^3/h = 720 kg/h (assume water density as 1000 kg/m^3) \) 2. Calculate the heat capacity rate of water: \( C_{water} = \dot{m}_{water} \times c_{p,water} = 720 kg/h \times 4180 J/kgK = 3011040 J/hK (assume specific heat capacity of water as 4180 J/kgK) \) Using the heat transfer equation: \( q = U A \Delta T_{lm} \) We have all variables except UA and \(\Delta T_{lm}\). So, we can use the heat capacity rate to find the required heat transfer, then use the LMTD method to determine the temperature difference, and finally calculate UA. Calculate the required heat transfer: \( q = \min(C_{milk},C_{water})\times(\Delta T_1-\Delta T_2) \). Since \(C_{milk}
02

Part B - Determine the Outlet Temperature of the Water

To find the outlet temperature of the water, we can use the following energy balance equation for water: \( \dot{m}_{water}c_{p,water}(T_{out,water} - T_{in,water}) = \dot{m}_{milk}c_{p,milk}(T_{in,milk} - T_{out,milk})\), where \(T_{in,water} = 10^{\circ}C\), \(T_{in,milk} = 38.6^{\circ}C\), and \(T_{out,milk} = 13^{\circ}C\). Now solve for \(T_{out,water}\): \(T_{out,water} = T_{in,water} + \frac{\dot{m}_{milk}c_{p,milk}(T_{in,milk} - T_{out,milk})}{\dot{m}_{water}c_{p,water}} \) \(T_{out,water} = 10 + \frac{257.5 \times 3860 (38.6 - 13)}{720 \times 4180} = 10 + 16.5 = 26.5^{\circ}C \) The outlet temperature of the water is 26.5°C.
03

Part C - Determine Milk Outlet Temperature for Different Water Flow Rates

To find the milk outlet temperature for different water flow rates, we can use the effectiveness-NTU method of heat exchanger analysis. The effectiveness (\(\epsilon\)) is defined as the actual heat transfer divided by the maximum possible heat transfer. First, we need to calculate the effectiveness of the original system when water flow rate is not changed: \(\epsilon = \frac{q}{\min(C_{milk}, C_{water})(T_{h, in} - T_{c, in})} = \frac{2982075}{994025 \times 28.6} = 0.979\) Now, let's examine the two scenarios: 1. If the water flow rate is doubled: \(\dot{m'}_{water} = 2 \times \dot{m}_{water} = 1440 kg/h\) Calculate the new heat capacity rate of water: \( C'_{water} = \dot{m'}_{water} \times c_{p, water} = 1440 kg/h \times 4180 J/kgK = 6022080 J/hK \) Since \(C_{milk}C''_{water}\), the heat transfer is determined by the capacity of water. Using the same effectiveness, we can calculate the new outlet temperature of milk: \(T''_{out,milk} = T_{in,milk} - \frac{\epsilon \times C''_{water}}{C_{milk}}(T_{in,milk}-T_{in,water}) = 38.6 - \frac{0.979 \times 1505520}{994025}(38.6 - 10) = 16.96^{\circ}C\) In conclusion, when the water flow rate is doubled, the milk outlet temperature is 13.97°C, and when the water flow rate is halved, the milk outlet temperature is 16.96°C.

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Key Concepts

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

Counterflow Heat Exchanger
Understanding a counterflow heat exchanger is critical when we talk about heat transfer systems. It's a type of heat exchanger where fluids move parallel to each other but in opposite directions. In our dairy operation example, the milk (hot fluid) and the groundwater (cold fluid) are flowing in opposing directions.

This configuration is highly efficient because it maintains a greater temperature difference between the fluids over the length of the heat exchanger, which drives the heat transfer. It's like a race where the hot and cold streams are running towards each other, and as they pass by, heat is exchanged. In this setup, the milk cools down significantly because it continually encounters colder water, as opposed to a co-current or parallel flow system where the temperatures of the two streams equalize quicker.

For the dairy operation, we maximize thermal efficiency by using this counterflow method. It allows us to reach the desired chilling temperature for the milk with a relatively short length of the exchanger, which we calculated to be about 7 meters. This is a fantastic application of physics and engineering to meet the needs of safe milk storage.
Log Mean Temperature Difference (LMTD)
Log Mean Temperature Difference, or LMTD, is a superb way to average the temperature difference between the hot and cold streams within a heat exchanger. It's not just an ordinary average; it's a logarithmic one, which smooths out the immediate ups and downs over the temperature gradient. To compute the LMTD, we focus on the difference in temperatures between the two fluids at each end of the heat exchanger.

The formula for LMTD is:
\[ \Delta T_{\text{lm}} = \frac{\Delta T_1 - \Delta T_2}{\ln(\frac{\Delta T_1}{\Delta T_2})} \]
Where \( \Delta T_1 \) and \( \Delta T_2 \) are the temperature differences at each end. In the case of the dairy operation, we used these values to solve for the LMTD and obtained 27.1°C. It's the LMTD that then allows us to determine how effectively our exchanger is doing its job by combining it with the overall heat transfer coefficient, U, to solve for the UA product. This step is essential because it ties the actual physical length required for the exchanger to the thermal performance needed for safe milk storage.
Effectiveness-NTU Method
When it comes to fine-tuning the performance of our heat exchanger, we employ the Effectiveness-NTU method. NTU stands for Number of Transfer Units, which reflects the heat exchanger’s size relative to the capacity rate of the fluids. Effectiveness, on the other hand, is the measure of how well the heat exchanger performs relative to its maximum potential. In essence, it tells us how close we are to the ideal scenario.

The formula that articulates this relationship is:
\[ \epsilon = \frac{q}{\min(C_{\text{milk}}, C_{\text{water}}) (T_{\text{h,in}} - T_{\text{c,in}})} \]
Where \( \epsilon \) is the effectiveness, \( q \) is the actual heat transfer, \( C \) is the heat capacity rate of each fluid, and \( T_{\text{h,in}} \) and \( T_{\text{c,in}} \) are the inlet temperatures of the hot and cold fluids.

Using this method, we can predict the impact of changing water flow rates on the cooling process, as was done for the dairy operation exercise. By understanding the effectiveness and how changing flow rates adjust heat capacity, it's like having a thermostat at our disposal. We controlled the milk's finished temperature by the flow rate and confirmed the effectiveness of our heat exchanger, ensuring that the milk reached safe storage temperature under different conditions.

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Most popular questions from this chapter

Ethylene glycol and water, at 60 and \(10^{\circ} \mathrm{C}\), respectively, enter a shell-and-tube heat exchanger for which the total heat transfer area is \(15 \mathrm{~m}^{2}\). With ethylene glycol and water flow rates of 2 and \(5 \mathrm{~kg} / \mathrm{s}\), respectively, the overall heat transfer coefficient is \(800 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\). (a) Determine the rate of heat transfer and the fluid outlet temperatures. (b) Assuming all other conditions to remain the same, plot the effectiveness and fluid outlet temperatures as a function of the flow rate of ethylene glycol for \(0.5 \leq \dot{m}_{h} \leq 5 \mathrm{~kg} / \mathrm{s}\).

In open heart surgery under hypothermic conditions, the patient's blood is cooled before the surgery and rewarmed afterward. It is proposed that a concentric tube, counterflow heat exchanger of length \(0.5 \mathrm{~m}\) be used for this purpose, with the thin-walled inner tube having a diameter of \(55 \mathrm{~mm}\). The specific heat of the blood is \(3500 \mathrm{~J} / \mathrm{kg} \cdot \mathrm{K}\). (a) If water at \(T_{h j}=60^{\circ} \mathrm{C}\) and \(\dot{m}_{h}=0.10 \mathrm{~kg} / \mathrm{s}\) is used to heat blood entering the exchanger at \(T_{c A}=18^{\circ} \mathrm{C}\) and \(\dot{m}_{c}=0.05 \mathrm{~kg} / \mathrm{s}\), what is the temperature of the blood leaving the exchanger? The overall heat transfer coefficient is \(500 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\). (b) The surgeon may wish to control the heat rate \(q\) and the outlet temperature \(T_{c, 0}\) of the blood by altering the flow rate and/or inlet temperature of the water during the rewarming process. To assist in the development of an appropriate controller for the prescribed values of \(\hat{m}_{c}\) and \(T_{c \jmath}\), compute and plot \(q\) and \(T_{c, \rho}\) as a function of \(\dot{m}_{h}\) for \(0.05 \leq \dot{m}_{\mathrm{h}} \leq 0.20 \mathrm{~kg} / \mathrm{s}\) and values of \(T_{h, l}=50,60\), and \(70^{\circ} \mathrm{C}\). Since the dominant influence on the overall heat transfer coefficient is associated with the blood flow conditions, the value of \(U\) may be assumed to remain at \(500 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\). Should certain operating conditions be excluded?

An automobile radiator may be viewed as a cross-flow heat exchanger with both fluids unmixed. Water, which has a flow rate of \(0.05 \mathrm{~kg} / \mathrm{s}\), enters the radiator at \(400 \mathrm{~K}\) and is to leave at \(330 \mathrm{~K}\). The water is cooled by air that enters at \(0.75 \mathrm{~kg} / \mathrm{s}\) and \(300 \mathrm{~K}\). (a) If the overall heat transfer coefficient is \(200 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\), what is the required heat transfer surface area? (b) A manufacturing engineer claims ridges can be stamped on the finned surface of the exchanger, which could greatly increase the overall heat transfer coefficient. With all other conditions remaining the same and the heat transfer surface area determined from part (a), generate a plot of the air and water outlet temperatures as a function of \(U\) for \(200 \leq U \leq 400 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\). What benefits result from increasing the overall convection coefficient for this application?

A shell-and-tube heat exchanger must be designed to heat \(2.5 \mathrm{~kg} / \mathrm{s}\) of water from 15 to \(85^{\circ} \mathrm{C}\). The heating is to be accomplished by passing hot engine oil, which is available at \(160^{\circ} \mathrm{C}\), through the shell side of the exchanger. The oil is known to provide an average convection coefficient of \(h_{o}=400 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\) on the outside of the tubes. Ten tubes pass the water through the shell. Each tube is thin walled, of diameter \(D=25 \mathrm{~mm}\), and makes eight passes through the shell. If the oil leaves the exchanger at \(100^{\circ} \mathrm{C}\), what is its flow rate? How long must the tubes be to accomplish the desired heating?

A two-fluid heat exchanger has inlet and outlet temperatures of 65 and \(40^{\circ} \mathrm{C}\) for the hot fluid and 15 and \(30^{\circ} \mathrm{C}\) for the cold fluid. Can you tell whether this exchanger is operating under counterflow or parallelflow conditions? Determine the effectiveness of the heat exchanger.

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