An aluminum plate of \(25 \mathrm{~mm}\) thick \((k=235 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K})\) is attached on a copper plate with thickness of \(10 \mathrm{~mm}\). The copper plate is heated electrically to dissipate a uniform heat flux of \(5300 \mathrm{~W} / \mathrm{m}^{2}\). The upper surface of the aluminum plate is exposed to convection heat transfer in a condition such that the convection heat transfer coefficient is \(67 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\) and the surrounding room temperature is \(20^{\circ} \mathrm{C}\). Other surfaces of the two attached plates are insulated such that heat only dissipates through the upper surface of the aluminum plate. If the surface of the copper plate that is attached to the aluminum plate has a temperature of \(100^{\circ} \mathrm{C}\), determine the thermal contact conductance of the aluminum/copper interface.

Short Answer

Expert verified
Question: Determine the thermal contact conductance of the aluminum/copper interface. Answer: To determine the thermal contact conductance of the aluminum/copper interface, follow these steps: 1. Calculate the heat dissipated through the aluminum plate: Q = Q_cond + Q_conv 2. Calculate the conduction heat transfer across the aluminum plate 3. Calculate the convection heat transfer at the upper surface of the aluminum plate 4. Relate the conduction and convection heat transfer through the aluminum plate 5. Calculate the heat transfer across the copper plate 6. Calculate the thermal contact conductance of the aluminum/copper interface using the formula: h_c = Q_Cu / ((T_Al_Copper - T_Cu_Surface) × A) By solving the problem following these steps, you can calculate the thermal contact conductance of the aluminum/copper interface.

Step by step solution

01

Calculate the heat dissipated through the aluminum plate

We know that heat generated by the copper plate is equal to heat transferred through the aluminum plate. The total heat transfer through the aluminum plate is given by the sum of the conduction heat transfer and the convection heat transfer: $$ Q = Q_{cond} + Q_{conv} $$
02

Calculate the conduction heat transfer across the aluminum plate

To find the conduction heat transfer through the aluminum plate, we can use the conduction equation with the known thermal conductivity, k = 235 W/m·K, and the thickness of the aluminum plate, L = 25 mm: $$ Q_{cond} = \frac{k \cdot A \cdot (T_{Al\ Copper} - T_{Al\ Surface})}{L} $$ Where \(T_{Al\ Copper}\) is the temperature at the aluminum/copper interface and \(T_{Al\ Surface}\) is the temperature at the upper surface of the aluminum plate. We need to find both temperatures to determine the conduction heat transfer.
03

Calculate the convection heat transfer at the upper surface of the aluminum plate

Using the given convection heat transfer coefficient, h = 67 W/m^2·K, we can calculate the convection heat transfer at the upper surface of the aluminum plate: $$ Q_{conv} = h \cdot A \cdot (T_{Al\ Surface} - T_{\infty}) $$ Where \(T_{\infty}\) refers to the surrounding room temperature, which is given as 20°C.
04

Relate the conduction and convection heat transfer through the aluminum plate

Combine and solve for the temperature at the aluminum/copper interface: $$ \frac{k \cdot A \cdot (T_{Al\ Copper} - T_{Al\ Surface})}{L} = Q_{cond} - h \cdot A \cdot (T_{Al\ Surface} - T_{\infty}) $$ We can solve this equation for the temperature at the aluminum/copper interface, \(T_{Al\ Copper}\).
05

Calculate the heat transfer across the copper plate

The heat flux generated in the copper plate is given as 5300 W/m². The heat transfer through the copper plate can be calculated using the heat flux: $$ Q_{Cu} = q' \cdot A $$ Where q' is the heat flux, and A is the area of the copper plate in contact with the aluminum plate.
06

Calculate the thermal contact conductance of the aluminum/copper interface

Now, we can calculate the thermal contact conductance (h_c) of the aluminum/copper interface. This is given by the following equation: $$ h_c = \frac{Q_{Cu}}{(T_{Al\ Copper} - T_{Cu\ Surface}) \cdot A} $$ Where \(T_{Cu\ Surface}\) is the temperature of the copper plate attached to the aluminum plate, which is given as 100°C. By substituting the values we know and solving for the thermal contact conductance, we can determine the aluminum/copper interface's thermal contact conductance. #Solution# To summarize, here are the steps to solve the problem: Step 1: Calculate the heat dissipated through the aluminum plate: Q = Q_cond + Q_conv Step 2: Calculate the conduction heat transfer across the aluminum plate Step 3: Calculate the convection heat transfer at the upper surface of the aluminum plate Step 4: Relate the conduction and convection heat transfer through the aluminum plate Step 5: Calculate the heat transfer across the copper plate Step 6: Calculate the thermal contact conductance of the aluminum/copper interface

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Key Concepts

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

Heat Transfer
Heat transfer is a fundamental concept in thermal physics and engineering, describing the movement of heat energy from one place to another. Heat can be transferred in three primary ways: conduction, convection, and radiation. In the context of the aluminum and copper plates exercise, the focus is on conduction and convection.

Conduction is the transfer of heat through a solid material, which occurs when molecules or atoms at a higher temperature energize neighboring particles. Thermal conductivity, denoted as 'k' in the exercise for aluminum (k=235 W/m·K), directly affects the rate of energy transfer, hence influencing how quickly or slowly heat moves through the material.

Convection, on the other hand, is the heat transfer that occurs within fluids (liquids and gases) due to the movement of the fluid itself. This process is influenced by the convection heat transfer coefficient 'h', which in this scenario is given as 67 W/m²·K. For the aluminum plate exposed at the top, the air around it acts as the fluid that either takes away or delivers heat to the plate through convective processes. Understanding these two mechanisms of heat transfer is critical in deriving an accurate solution for the aluminum/copper interface's thermal contact conductance.
Conduction and Convection
In a scenario where two different metals are in contact, such as aluminum and copper plates in the exercise, heat conduction at their interface becomes a key area of focus. The heat must first conduct through one metal and then transfer to the other, each with their own characteristic thermal conductivity values.

The formula for calculating conduction heat transfer is given by Fourier's law of conduction, as shown in the solution steps: $$Q_{cond} = \frac{k \cdot A \cdot (T_{Al\_Copper} - T_{Al\_Surface})}{L}$$
On the surface of the aluminumplate exposed to air, convection plays a role. The convection heat transfer can be calculated using the formula: $$Q_{conv} = h \cdot A \cdot (T_{Al\_Surface} - T_{\infty})$$where 'h' is the heat transfer coefficient and 'T_{\infty}' is the surrounding temperature.

Exercise Improvement Advice

It's essential to provide clarity on the relationship between conduction and convection in the heat dissipation process. Stating that the heat generated by the copper plate must equal the heat lost by the aluminum plate through conduction and convection could enhance comprehension. Additionally, depicting the path of heat flow with diagrams could visually reinforce the understanding of these concepts.
Thermal Conductivity
Thermal conductivity, denoted as 'k' in physical equations, is a measure of a material's ability to conduct heat. The unit Watt per meter-Kelvin (W/m·K) indicates how much heat in Watts can be transferred through a meter-thick sample of the material when there is a temperature difference of one Kelvin across the sample. In our exercise, the aluminum plate has a thermal conductivity of 235 W/m·K, meaning it is quite good at conducting heat.

Factors that impact thermal conductivity include the material's composition, temperature, and phase (solid, liquid, or gas). Metals, such as aluminum and copper, typically have higher thermal conductivity because their delocalized electrons can transfer kinetic energy quickly between atoms.

The thermal conductivity comes into play when determining the temperature drop across a material and influences how efficiently heat can be transferred from the interface. As part of the solution process, it has been used to calculate the rate of heat conduction through the aluminum plate. This property, along with the thickness of the material, directly impacts the thermal contact conductance, which is essential for engineering applications where heat dissipation is critical, such as in computer processors or mechanical systems.

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Most popular questions from this chapter

Steam at \(450^{\circ} \mathrm{F}\) is flowing through a steel pipe \(\left(k=8.7 \mathrm{Btu} / \mathrm{h} \cdot \mathrm{ft} \cdot{ }^{\circ} \mathrm{F}\right)\) whose inner and outer diameters are \(3.5\) in and \(4.0\) in, respectively, in an environment at \(55^{\circ} \mathrm{F}\). The pipe is insulated with 2 -in-thick fiberglass insulation \((k=\) \(\left.0.020 \mathrm{Btu} / \mathrm{h} \cdot \mathrm{ft} \cdot{ }^{\circ} \mathrm{F}\right)\). If the heat transfer coefficients on the inside and the outside of the pipe are 30 and \(5 \mathrm{Btu} / \mathrm{h} \cdot \mathrm{ft}^{2} \cdot{ }^{\circ} \mathrm{F}\), respectively, determine the rate of heat loss from the steam per foot length of the pipe. What is the error involved in neglecting the thermal resistance of the steel pipe in calculations?

Obtain a relation for the fin efficiency for a fin of constant cross-sectional area \(A_{c}\), perimeter \(p\), length \(L\), and thermal conductivity \(k\) exposed to convection to a medium at \(T_{\infty}\) with a heat transfer coefficient \(h\). Assume the fins are sufficiently long so that the temperature of the fin at the tip is nearly \(T_{\infty}\). Take the temperature of the fin at the base to be \(T_{b}\) and neglect heat transfer from the fin tips. Simplify the relation for \((a)\) a circular fin of diameter \(D\) and \((b)\) rectangular fins of thickness \(t\).

In the United States, building insulation is specified by the \(R\)-value (thermal resistance in \(\mathrm{h} \cdot \mathrm{ft}^{2} \cdot{ }^{\circ} \mathrm{F} /\) Btu units). A homeowner decides to save on the cost of heating the home by adding additional insulation in the attic. If the total \(R\)-value is increased from 15 to 25 , the homeowner can expect the heat loss through the ceiling to be reduced by (a) \(25 \%\) (b) \(40 \%\) (c) \(50 \%\) (d) \(60 \%\) (e) \(75 \%\)

Heat is generated steadily in a 3-cm-diameter spherical ball. The ball is exposed to ambient air at \(26^{\circ} \mathrm{C}\) with a heat transfer coefficient of \(7.5 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\). The ball is to be covered with a material of thermal conductivity \(0.15 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\). The thickness of the covering material that will maximize heat generation within the ball while maintaining ball surface temperature constant is (a) \(0.5 \mathrm{~cm}\) (b) \(1.0 \mathrm{~cm}\) (c) \(1.5 \mathrm{~cm}\) (d) \(2.0 \mathrm{~cm}\) (e) \(2.5 \mathrm{~cm}\)

Two finned surfaces are identical, except that the convection heat transfer coefficient of one of them is twice that of the other. For which finned surface is the \((a)\) fin effectiveness and \((b)\) fin efficiency higher? Explain.

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