/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 135 As a means of enhancing heat tra... [FREE SOLUTION] | 91Ó°ÊÓ

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As a means of enhancing heat transfer from highperformance logic chips, it is common to attach a heot sink to the chip surface in order to increase the surface area available for convection heat transfer. Because of the ease with which it may be manufactured (by taking orthogonal sawcuts in a block of material), an attmctive option is to use a heat sink consisting of an atmy of square fins of width w on s side. The spacing between adjoining fins would be determined by the width of the sawblade, with the sum of this spacing and the fan width designated as the fin pitch \(S\). The method by which the hent sink is joined to the chip would detesmine the interfacial contact resistance, \(R_{\mathcal{U}^{*}}^{*}\) Consider a square chip of width \(W_{c}=16 \mathrm{~mm}\) and conditions for which cooling is provided by a diclectric liquid with \(T_{w}=25^{\circ} \mathrm{C}\) and \(h=1500 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\). The heat sink is fahricated from copper \((k=400\) Whe \(\mathrm{K})\), and its characteristic dimensions are \(w=0.25\) \(\operatorname{mmn}_{,} S=0.50 \mathrm{~mm}, L_{y}=6 \mathrm{~mm}\), and \(L_{1}=3 \mathrm{~mm}\). The preccribed values of \(w\) and \(S\) represent minima imposed by manufacturing constraints and the need to maintain adequate flow in the passages between fins. (a) If a metallurgical joint provides a contact resistance of \(R_{\mathrm{W}}^{*}=5 \times 10^{-6} \mathrm{~m}^{2}+\mathrm{K} / \mathrm{W}\) and the maximum allowable chip temperature is \(85^{\circ} \mathrm{C}\), what is the maximum allowable chip power dissipation \(q, ?\) Assume all of the heat to be transferred through the heat sink. (b) It may be possible to increase the heat dissipation by increasing \(w\), subject to the constraint that \((S-w) \geq 0.25 \mathrm{~mm}\), and/or increasing \(L_{f}\) (suhject to manufacturing constraints that \(L_{y} \leq 10 \mathrm{~mm}\). Assess the effect of such changes.

Short Answer

Expert verified
The maximum chip power dissipation is determined by thermal resistance; modify fin dimensions for improved results.

Step by step solution

01

Calculate Thermal Resistance Components

First, calculate the thermal resistance through the heat sink, which includes conduction through the fins and convection from the fins to the liquid. Use the formula for fin efficiency and the convective thermal resistance \( R_{th} = \frac{1}{{n * \eta_f * A_f * h}} \), where \( n \) is the number of fins, \( \eta_f \) is the fin efficiency, \( A_f \) is the fin area, and \( h \) is the convection coefficient.
02

Determine Fin Efficiency

Calculate the efficiency of the fins using\( \eta_f = \tanh(mL_f)/(mL_f) \),where \( m = \sqrt{{2h}/{kAf}} \), \( Af \) is the fin cross-sectional area, and \( k \) is the conductivity of copper. Substitute the known values to find \( \eta_f \).
03

Calculate Overall Thermal Resistance

Sum the individual thermal resistances including the interfacial contact resistance \( R_{total} = R_{cu} + R_{conv} + R_{\text{contact}} \). Use the values from the previous steps to find \( R_{total} \).
04

Determine Heat Dissipation

Using the calculated total thermal resistance, compute the power dissipation using the formula \( q = \frac{(T_{max} - T_w)}{R_{total}} \),where \( T_{max} = 85^{\circ} \text{C} \) and \( T_w = 25^{\circ} \text{C} \).
05

Evaluate Effects of Changing Parameters

Consider changes in \( w \) and \( L_f \) to increase heat dissipation according to \( q = \frac{(T_{max} - T_w)}{R_{total}(w, L_f)} \).Recalculate \( q \) with these adjusted parameters while considering the constraints on spacing \((S-w)\) and fin length \(L_f \).

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Key Concepts

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

Thermal Resistance
Thermal resistance is a crucial concept in heat transfer, especially when dealing with systems like heat sinks. It represents the system’s resistance to heat flow through different materials or interfaces, akin to how electrical resistance operates in a circuit. In the case of a heat sink attached to a high-performance chip, understanding thermal resistance allows us to measure how effectively heat can dissipate from the chip’s surface into the surrounding medium, which is often a liquid or air. Thermal resistance is cumulative and consists of several components:
  • Conduction Resistance: This is the resistance against heat flow through solid materials, such as the copper fins in the heat sink. It depends on the material's properties and geometric dimensions.
  • Convection Resistance: This resistance represents the heat transfer to a fluid, like air or a dielectric liquid, surrounding the heat sink. It's influenced by factors like the convection coefficient, surface area, and the effectiveness of fin design.
  • Interfacial Resistance: The thermal resistance at the contact point between the chip and the heat sink, which can be minimized using high-quality joints.
Each component adds up to create the total thermal resistance for the system, which should be minimized to enhance cooling.
Fin Efficiency
Fin efficiency is a measurement of how effectively a fin transfers heat from its base into the surrounding fluid. Ideally, a fin would have an efficiency of 100%, indicating perfect heat transfer, but real fins often fall short due to several heat losses.The efficiency of a fin depends on various factors:
  • Material: Conductivity plays a major role. High conductivity materials like copper are preferred for manufacturing fins.
  • Geometry: The shape and size of a fin affect how heat spreads throughout the material. For instance, longer or thinner fins usually aid in better heat distribution.
  • Environmental Conditions: The convection coefficient of the surrounding environment impacts how effectively heat is exchanged between the fin and the surrounding fluid.
To calculate fin efficiency, we use the formula: \[ \eta_f = \frac{\tanh(mL_f)}{mL_f} \]Where \( m = \sqrt{\frac{2h}{kA_f}} \), and \( A_f \) is the cross-sectional area of the fin. Here, \( m \) represents how swiftly heat can travel within the fin material. Understanding fin efficiency helps in evaluating a heat sink's performance and suggests ways to improve heat dissipation by tweaking fin parameters.
Heat Dissipation
Heat dissipation refers to the process by which heat is expelled from an area, such as a computer chip, preventing overheating and maintaining optimal functionality. In heat sinks, this process predominantly relies on enhancing the thermal pathway from the chip to the surrounding cooling medium via convection and conduction.The rate of heat dissipation is influenced by elements such as:
  • Overall Thermal Resistance: Lower thermal resistance facilitates better heat flow through the heat sink.
  • Heat Sink Design: Factors like the number of fins, their size, and their placement affect the overall heat transfer rate.
  • Ambient Conditions: The temperature difference between the chip and the cooling fluid (\( T_{max} - T_w \)) drives the rate of dissipation.
The formula used for calculating the power dissipation is: \[ q = \frac{(T_{max} - T_w)}{R_{total}} \]By minimizing \( R_{total} \), and optimizing factors like fin size and material, engineers can maximize \( q \), increasing the chip's power capacity without risking overheating. Adjustments in fin dimensions or material properties can significantly impact \( q \), making the understanding of heat dissipation critical in design and performance assessment.
Interfacial Contact Resistance
Interfacial Contact Resistance is the restriction to heat flow at the interface where two bodies meet, such as the chip and the heat sink. Despite seeming minor, this resistance can significantly impact the effectiveness of heat dissipation in electronic systems, as it acts as a bottleneck for heat transfer.Contact resistance is typically influenced by:
  • Material Mismatch: Different thermal properties of contact materials can create inefficiencies.
  • Surface Roughness: The smoother the contact surfaces, the better the thermal interface between them. Rough or uneven surfaces trap air pockets that act as insulators.
  • Bonding Quality: Better bonds, such as those made through metallurgical joining, can offer lower contact resistance compared to adhesive or mechanical joints.
For the given exercise, the interfacial contact resistance \( R_{\text{contact}} \) was specified and needs to be taken into account when calculating the total resistance: \[ R_{total} = R_{cu} + R_{conv} + R_{\text{contact}} \]By aiming to minimize this resistance, the heat transfer from the chip to the heat sink interface can be optimized, thus maintaining lower chip temperatures and enhancing performance.

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Most popular questions from this chapter

A plane wall of thickness \(0.1 \mathrm{~m}\) and thermal conductiv ity \(25 \mathrm{~W} / \mathrm{m}\), K having uniform volumetric heat generation of \(0.3 \mathrm{MW} / \mathrm{m}^{3}\) is insulated on one side, while the other side is exposed to a fluid at \(92^{\circ} \mathrm{C}\). The convection heat transfer coefficient between the wall and the fluid is \(500 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\). Determine the maximum temperature in the wall.

Aluminum fins of triangular profile are attached to a plane wall whose surface temperature is \(250^{\circ} \mathrm{C}\). The fin base thickness is \(2 \mathrm{~mm}\), and its length is \(6 \mathrm{~mm}\). The system is in ambient air at a temperature of \(20^{\circ} \mathrm{C}\), and the surface convection coefficient is \(40 \mathrm{~W} / \mathrm{m}^{2}+\mathrm{K}\). (a) What are the fin efficiency and effectiveness? (b) What is the heat dissipated per unit width by a single fin?

Radinactive wastes \(\left(k_{1 w}=20 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\right)\) are stored in a spherical, stainless steel \(\left(k_{\mathrm{m}}=15 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\right)\) container of inner and outer radii equal to \(r_{i}=0.5 \mathrm{~m}\) and \(r_{e}=0.6 \mathrm{~m}\). Heat is genersed volumetrically within the wastes at a unifom rate of \(\hat{q}=10^{8} \mathrm{~W} / \mathrm{m}^{3}\), and the outer surface of the container is exposed to a water flow for which \(h=\) \(1000 \mathrm{~W} / \mathrm{m}^{2}-\mathrm{K}\) and \(T_{\mathrm{s}}=25^{\circ} \mathrm{C}\).

A composite wall separates combustion gases at \(2600^{\circ} \mathrm{C}\) from a liquid coolant at \(100^{\circ} \mathrm{C}\), with gas- and liquid-side convection coefficients of 50 and 1000 \(W / \mathrm{m}^{2} \cdot \mathbf{K}\). The wall is composed of a 10 -mm-thick layer of beryllium oxide on the gas side and a 20 -mm-thick slab of stainless steel (AISI 304) on the liquid side. The contact resistance between the oxide and the steel is \(0.05 \mathrm{~m}^{2} \cdot \mathrm{K} / \mathrm{W}\). What is the heat loss per unit surface area of the composite? Sketch the temperature distribution from the gas to the liquid.

A spherical vessel used as a reactor for producing pharmaceuticals has a 10 -mam-thick stainless steel wall \((k=\) \(17 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K})\) and an inner diameter of \(1 \mathrm{~m}\). The exteria surface of the vessel is exposed to ambient air \(\left(T_{z}=\right.\) \(25^{\circ} \mathrm{C}\) ) for which a convection coefficient of \(6 \mathrm{~W} / \mathrm{m}^{2}+\mathrm{K}\) may be assumed. (a) During steady-state operation, an inner surfact temperature of \(50^{\circ} \mathrm{C}\) is maintained by enengy geneated within the reactor. What is the heat loss from the vessel? (b) If a 20-mm-thick layer of fiberglass insulation \((k=\) \(0.040 \mathrm{~W} / \mathrm{m}\) - K) is applied to the exterior of the ve sel and the rate of thermal energy generation is inchanged, what is the inner surface temperature of the vessel?

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