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	<title>heat transfer Archives - Boyd | Trusted Innovation</title>
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	<title>heat transfer Archives - Boyd | Trusted Innovation</title>
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		<title>The Best Heat Transfer Fluids for Liquid Cooling</title>
		<link>https://www.boydcorp.com/blog/best-heat-transfer-fluids.html</link>
		
		<dc:creator><![CDATA[Boyd Blog]]></dc:creator>
		<pubDate>Tue, 24 May 2022 12:53:44 +0000</pubDate>
				<category><![CDATA[Blog]]></category>
		<category><![CDATA[Liquid Cooling]]></category>
		<category><![CDATA[Material Science]]></category>
		<category><![CDATA[Thermal]]></category>
		<category><![CDATA[fluids]]></category>
		<category><![CDATA[heat transfer]]></category>
		<category><![CDATA[liquid cooling system]]></category>
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					<description><![CDATA[<p>The post <a href="https://www.boydcorp.com/blog/best-heat-transfer-fluids.html">The Best Heat Transfer Fluids for Liquid Cooling</a> appeared first on <a href="https://www.boydcorp.com">Boyd | Trusted Innovation</a>.</p>
]]></description>
										<content:encoded><![CDATA[<div class="et_pb_section et_pb_section_0 et_section_regular" >
				
				
				
				
				
				
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				<div class="et_pb_text_inner"><p>Once you’ve determined liquid cooling is the solution, do you know what heat transfer fluid to use? One of the most important factors when choosing a liquid cooling technology for your application is the compatibility of the heat transfer fluid with the wetted surfaces of each part of liquid cooling loop. This includes <a href="https://www.boydcorp.com/thermal/liquid-cooling-systems/liquid-cold-plates.html">liquid cold plates</a>, <a href="https://www.boydcorp.com/thermal/liquid-cooling-systems/heat-exchangers.html">heat exchangers</a>, <a href="https://www.boydcorp.com/thermal/liquid-cooling-systems/coolant-distribution-unit-cdu.html">CDUs</a>, <a href="https://www.boydcorp.com/engineered-materials/environmental-sealing-protection/liquid-airflow-management.html">tubes</a>, and any quick disconnects.</p></div>
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				<div class="et_pb_text_inner"><h2>Introduction to Common Liquids for Cooling Systems</h2>
<p>Long-term liquid cooling system reliability depends on heat transfer fluid compatibility. Other heat transfer fluid requirements may include high thermal conductivity, specific heat, low viscosity, low freezing point, high flash point, low corrosivity, low toxicity, and thermal stability. Based on these criteria, the most commonly used coolants for liquid cooling applications today are:</p>
<ul>
<li>Water</li>
<li>Deionized Water</li>
<li>Inhibited Glycol and Water Solutions</li>
<li>Dielectric Fluids</li>
</ul></div>
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				<span class="et_pb_image_wrap "><img decoding="async" width="566" height="300" src="https://www.boydcorp.com/wp-content/uploads/Resources/Blog/Introduction-to-Common-Liquids-for-Cooling-Systems-566x300-1.jpg" alt="Common Liquids for Cooling Systems" title="" class="wp-image-14725" /></span>
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				<div class="et_pb_text_inner"><p>By selecting a compatible pairing of heat transfer fluid and wetted materials, you’ll minimize the risk of corrosion and optimize thermal performance.</p>
<p><strong>Copper is compatible with water and glycol/water solutions.</strong></p>
<p><strong>Aluminum is compatible with glycol/water solutions, dielectric fluids, and oils.</strong></p>
<p><strong>Stainless steel is better for deionized water or other corrosive fluids because of its improved corrosion resistance over other metals.</strong></p>
<p>Most cooling systems are compatible with water or glycol/water solutions but require specialized plumbing for deionized water or a dielectric fluid like polyalphaolefin (PAO).</p></div>
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				<div class="et_pb_text_inner"><h2>Materials &amp; Fluid Compatibility</h2></div>
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<table id="tablepress-34" class="tablepress tablepress-id-34">
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	<th class="column-1">Metal</th><th class="column-2">Water</th><th class="column-3">Glycol</th><th class="column-4">Deionized</th><th class="column-5">Dielectric Fluids<br />
(Fluorinert, PAO)</th>
</tr>
</thead>
<tbody class="row-striping row-hover">
<tr class="row-2">
	<td class="column-1">Copper</td><td class="column-2">X</td><td class="column-3">X</td><td class="column-4"></td><td class="column-5">X</td>
</tr>
<tr class="row-3">
	<td class="column-1">Aluminum</td><td class="column-2">X</td><td class="column-3"></td><td class="column-4">X</td><td class="column-5"></td>
</tr>
<tr class="row-4">
	<td class="column-1">Stainless Steel</td><td class="column-2">X</td><td class="column-3">X</td><td class="column-4">X</td><td class="column-5">X</td>
</tr>
</tbody>
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				<div class="et_pb_text_inner"><h2>Water as a Heat Transfer Fluid</h2></div>
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				<span class="et_pb_image_wrap "><img decoding="async" width="566" height="300" src="https://www.boydcorp.com/wp-content/uploads/Resources/Blog/Water-as-a-Heat-Transfer-Fluid-566x300-1.jpg" alt="Water as a Heat Transfer Fluid" title="" class="wp-image-14729" /></span>
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				<div class="et_pb_text_inner"><p>Water is one of the best choices for liquid cooling applications due to its high heat capacity and thermal conductivity. It is also compatible with copper, which is one of the best heat transfer materials to use for your fluid path.</p></div>
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				<div class="et_pb_text_inner"><h3>Facility Water or Tap Water</h3>
<p>Water for liquid cooling comes from different sources. Tap water, for example, comes from a publicly owned water treatment facility or a well. The benefit to using facility or tap water is that it is readily available and inexpensive. What is important to note about facility water or tap water is that it is likely untreated and likely to contain impurities. Impurities can cause corrosion in the liquid cooling loop and/or clog fluid channels. Therefore, using good quality water is recommended to minimize corrosion and optimize thermal performance.</p></div>
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				<div class="et_pb_text_inner"><h3>Water’s Potential for Corrosion</h3>
<p>Water’s ability to corrode metal can vary considerably depending on its chemical composition. Corrosive chloride is commonly found in tap water. Facility or tap water should not be used in liquid cooling loops if it contains more than 25 PPM of chloride.</p>
<p>The levels of calcium and magnesium in the water also need to be considered. Calcium and magnesium can form scale on metal surfaces and reduce the thermal performance of the components.</p></div>
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				<div class="et_pb_text_inner"><h2>Water Liquid Cooling Recommended Limit of Minerals</h2></div>
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	<th class="column-1">Mineral</th><th class="column-2">Recommended Limit</th>
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	<td class="column-1">Calcium</td><td class="column-2">< 50 ppm</td>
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	<td class="column-1">Chloride</td><td class="column-2">< 25 ppm</td>
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	<td class="column-1">Magnesium</td><td class="column-2">< 50 ppm</td>
</tr>
<tr class="row-5">
	<td class="column-1">Sulfate</td><td class="column-2">< 25 ppm</td>
</tr>
<tr class="row-6">
	<td class="column-1">Total Hardness</td><td class="column-2">< 100 ppm (5 grains)</td>
</tr>
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				<div class="et_pb_text_inner"><h3>Deionized Water or Filtered Water</h3>
<p>If your facility water or tap water contains a large percent of minerals, salts, or other impurities, you can either filter the water or purchase filtered or deionized water.</p></div>
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				<div class="et_pb_text_inner"><h3>Corrosion Inhibitors: Phosphate, Tolyltriazole, and Organic Acids</h3>
<p>We still recommend using a corrosion inhibitor for additional protection even if your facility or tap water is relatively pure and meets recommended limits. Phosphate is an effective corrosion inhibitor for stainless steel and most aluminum components. It’s also effective for pH control. One disadvantage of phosphate is that it precipitates with calcium in hard water. For copper and brass, tolyltriazole is a common and highly effective corrosion inhibitor. For aluminum, organic acids such as 2-ethyl hexanoic or sebacic acid offer protection.</p></div>
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				<div class="et_pb_text_inner"><h2>Deionized Water</h2>
<p>Deionized water is water that has had its ions removed, including sodium, calcium, iron, copper, chloride, and bromide. The deionization process removes harmful minerals, salts, and other impurities that can cause corrosion or scale formation. Compared to tap water and most other fluids, deionized water has a high resistivity. Deionized water is an excellent insulator which is ideal for electrical components manufacturing or immersion cooling where components bust be electrically isolated.</p></div>
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				<span class="et_pb_image_wrap "><img decoding="async" width="566" height="300" src="https://www.boydcorp.com/wp-content/uploads/Resources/Blog/Deionized-Water-566x300-1.jpg" alt="Deionized Water" title="" class="wp-image-14731" /></span>
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				<div class="et_pb_text_inner"><h3>Corrosivity of Deionized Water</h3>
<p>However, as water’s resistivity increases, its corrosivity increases as well. Deionized water is approximately pH 7.0 but will quickly become acidic when exposed to air. The carbon dioxide in air dissolves in the water, introducing ions and reduces the pH to 5.0. Corrosion inhibitors are required when using virtually pure water. When using deionized water in a recirculating chiller or CDU, special high purity plumbing are a must. The fittings should be nickel-plated and the evaporators should be nickel-brazed. When using deionized water in cold plates or heat exchangers, stainless steel tubing is recommended.</p></div>
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				<div class="et_pb_text_inner"><h3>Pros to Deionized Water in Liquid Cooling Systems</h3>
<p>Tap water meets the needs of most liquid-cooling applications. However, deionized (DI) water has chemical and electrical properties that make it the optimal choice for cooling when the liquid circuit contains micro-channels or when sensitive electronics are involved.</p>
<p>DI water has an extremely low concentration of ions which defines important performance attributes. First, it eliminates mineral deposits which block coolant flow which degrade cooling efficiency and system operating performance. Second, it eliminates the risk of electrical arcing due to static charge build-up from the circulating coolant. Arcing can damage sensitive control electronics in the cooled equipment. No ions in DI water eliminates both problems.</p></div>
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				<div class="et_pb_text_inner"><h2>How to use Deionized Water in a Liquid Cooling System</h2>
<p>Applications that need DI water are found in industries such as:</p>
<ul>
<li>Medical equipment</li>
<li>Laboratory instrumentation</li>
<li>Pharmaceutical production and food processing</li>
<li>Cosmetic</li>
<li>Semiconductor manufacturing</li>
<li>Lasers, plating, chemical and other industrial processing</li>
</ul>
<p>Exercise care when using DI water. The lack of ions makes this coolant unusually corrosive. Called the “universal solvent,” deionized water is one of the most aggressive solvents known. It will dissolve everything to which it is exposed to varying degrees. Therefore all materials in the cooling loop must be corrosion-resistant.</p></div>
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				<div class="et_pb_text_inner"><h3>Copper’s Non-compatibility with Deionized Water</h3>
<p>Copper and many other common materials are not compatible with DI water and will contaminate it. When you design a system using DI water, be sure to specify DI-compatible materials such as stainless steel or nickel.</p></div>
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				<div class="et_pb_text_inner"><h3>Stainless Steel Wetted Paths for Deionized Water</h3>
<p>In a heat exchanger or cold plate, we recommend a stainless steel fluid path. A DI friendly <a href="https://www.boydcorp.com/thermal/liquid-cooling-systems/chillers.html">recirculating chiller</a> should contain a nickel-brazed evaporator, a stainless steel pump head, and nickel-plated fittings. Finally, to maintain DI water purity, a deionization cartridge must be included. As with all consumables the DI cartridge must be replaced periodically.</p>
<p>In summary, many types of equipment and applications require DI water-cooled systems. When properly designed and maintained, these systems can provide reliable cooling and leak-free operation for many years.</p></div>
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				<div class="et_pb_text_inner"><h2>Inhibited Glycol and Water Solutions in Liquid Cooling</h2></div>
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				<span class="et_pb_image_wrap "><img decoding="async" width="566" height="300" src="https://www.boydcorp.com/wp-content/uploads/Resources/Blog/Inhibited-Glycol-and-Water-Solutions-in-Liquid-Cooling-566x300-1.jpg" alt="Inhibited Glycol and Water Solutions in Liquid Cooling" title="" class="wp-image-14733" /></span>
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				<div class="et_pb_text_inner"><p>The two types of glycol most commonly used for liquid cooling applications are ethylene glycol and water (EGW) and propylene glycol and water (PGW) solutions.</p></div>
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				<div class="et_pb_text_inner"><h3>Ethylene Glycol and Water</h3>
<p>Ethylene glycol has desirable thermal properties including a high boiling point, low freezing point, stability over a wide range of temperatures, and high specific heat and thermal conductivity. It also has low viscosity, meaning reduced pumping requirements. Even though EGW’s thermal conductivity is not as high as water it provides freeze protection that can be beneficial during use or shipping.</p></div>
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				<div class="et_pb_text_inner"><h3>Propylene Glycol and Water</h3>
<p>Although EGW has more desirable physical properties than PGW, propylene glycol/water is used in applications where toxicity might be a concern. PGW is generally recognized as safe for use in food or food processing applications and can also be used in enclosed spaces.</p></div>
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				<div class="et_pb_text_inner"><h3>Automotive Ethylene Glycol and Water</h3>
<p>Ethylene glycol is used in automotive antifreeze. However, automotive glycol should not be used in a cooling system or heat exchanger because it contains silicate-based rust inhibitors. These inhibitors can gel and foul, coating heat exchanger surfaces and reducing their efficiency. Silicates have also been shown to significantly reduce the lifespan of pump seals.</p></div>
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				<div class="et_pb_text_inner"><h3>Choosing the Right Rust Inhibitor for Glycol and Water Solutions</h3>
<p>While the wrong inhibitors can cause significant problems, the right inhibitors can prevent corrosion and significantly prolong the life of a liquid cooling loop. Inhibited glycols can be purchased from specialized fluid production companies and are highly recommended over non-inhibited glycols.</p></div>
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				<div class="et_pb_text_inner"><h3>Glycol Concentration</h3>
<p>As the concentration of glycol in the solution increases, the thermal performance of the heat transfer fluid decreases. Use the lowest possible concentration of inhibited glycol necessary to meet your corrosion and freeze protection needs. Dow Chemical recommends a minimum concentration of 25-30% EGW4. At this minimum concentration, ethylene glycol also serves as a bactericide and fungicide. With recirculating chillers, a solution of 30% ethylene glycol will result in only about a 3% drop in thermal performance over using water alone but will provide corrosion protection as well as freeze protection down to -15°C (5°F).</p></div>
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				<div class="et_pb_text_inner"><h3>Water Quality in Glycol Solutions</h3>
<p>The quality of the water used in the glycol solution is also important. The water should meet or exceed the limits specified in the Recommended Mineral Limit table, even if you’re using an inhibited glycol. Ions in the water can cause the inhibitor to fall out of solution, resulting in fouling and corrosion.</p></div>
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				<div class="et_pb_text_inner"><h2>Adding Glycol into your Liquid Coolant</h2></div>
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				<span class="et_pb_image_wrap "><img decoding="async" width="1215" height="300" src="https://www.boydcorp.com/wp-content/uploads/Resources/Blog/Adding-Glycol-into-your-Liquid-Coolant-1215x300-1.jpg" alt="Adding Glycol into your Liquid Coolant" title="" class="wp-image-14738" /></span>
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				<div class="et_pb_text_inner"><h3>When Is It Necessary to Add Glycol in Your Coolant?</h3>
<p>Boyd recommends using a 30/70 glycol-water mixture with its recirculating chillers whenever the coolant temperature set point is below 10°C (48°F). Glycol lowers the freezing point of the mixture *(Figure 1). Adding glycol to your coolant reduces the freezing point of the coolant to around -34°C, preventing any risk of damage to your chiller caused by freezing.</p>
<p>Glycol does not transfer heat as well as pure water (Fig. 2 &amp; 3). So if there is no risk of freezing, use 100% water as adding glycol to your system will decrease performance. However, when the set point is below 10°C (48°F) there is a risk of freezing and Glycol should be added to water. The slight decrease in performance is a necessary trade-off to safely allow the lower temperature set point.</p></div>
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				<span class="et_pb_image_wrap "><img decoding="async" width="261" height="356" src="https://www.boydcorp.com/wp-content/uploads/Resources/Blog/Freezing-Point-with-Dowcal-Graph.jpg" alt="Figure 1: Graph illustrating freezing point of aqueous solution of DOWCAL 10" title="" class="wp-image-13844" /></span>
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				<span class="et_pb_image_wrap "><img decoding="async" width="684" height="316" src="https://www.boydcorp.com/wp-content/uploads/Resources/Blog/Specific-Heat-Thermal-Conductivity-with-Dowcal-Graphs.jpg" alt="Specific Heat Thermal Conductivity with Dowcal Graphs" title="Figure 2: Graph illustrating specific heat of aqueous solutions of DOWCAL 10 fluid. Figure 3: Graph illustrating thermal conductivity of aqueous solution of DOWCAL 10 fluid." class="wp-image-13845" /></span>
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				<div class="et_pb_text_inner"><h3>How Coolants Work in Chillers</h3>
<p>In a recirculating chiller, the liquid coolant flows through the application, removing excess heat and raising the temperature of the liquid. This coolant then needs to be returned to set point temperature by flowing through a heat exchanger called the evaporator.</p>
<p>Learn more about <a href="https://www.boydcorp.com/blog/compressor-based-refrigeration-basics.html">Compressor-Based Refrigeration</a>.</p></div>
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				<div class="et_pb_text_inner"><p>The heat exchanger transfers heat between the liquid coolant and the system’s refrigerant gas. The refrigerant’s temperature must be lower than the temperature of coolant liquid for heat to flow and for coolant temperature to be effectively returned to set point.</p>
<p>The temperature of the refrigerant is typically 5°C to 10°C lower than coolant temperature to allow heat to flow. Consequently, if the temperature set point is below 10°C (48°F), the refrigerant’s temperature can be close to, or even below the freezing point of water. If the coolant freezes, the evaporator can become obstructed, preventing water flow. Water expands as it freezes, which can permanently damage the evaporator.</p></div>
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				<div class="et_pb_text_inner"><h2>Dielectric Fluids</h2>
<p>Power electronics, laser, and semiconductor industries might be more likely to choose dielectric fluids over water. A dielectric fluid is non-conductive and preferred over water when working with sensitive electronics.</p></div>
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				<span class="et_pb_image_wrap "><img decoding="async" width="566" height="300" src="https://www.boydcorp.com/wp-content/uploads/Resources/Blog/Dielectric-Fluids-566x300-1.jpg" alt="Dielectric Fluids" title="" class="wp-image-14742" /></span>
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				<div class="et_pb_text_inner"><h3>Perfluorinated Carbons as a Heat Transfer Fluid</h3>
<p>Perfluorinated carbons, such as 3M’s dielectric fluid Fluorinert™, are non-flammable, non-explosive, and thermally stable over a wide range of operating temperatures. Although deionized water is also non-conductive, Fluorinert™ is less corrosive than deionized water and therefore may be a better choice for some applications. However, water has a thermal conductivity of approximately 0.59 W/m°C (0.341 BTU/hr ft °F), while Fluorinert™ FC-77 has a thermal conductivity of only about 0.063 W/m°C (0.036 BTU/hr ft °F). Fluorinert™ is also much more expensive than deionized water.</p></div>
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				<div class="et_pb_text_inner"><h3>Polyalphaolefin Liquid Cooling</h3>
<p>PAO is a synthetic hydrocarbon used frequently in defense and aerospace applications for its dielectric properties and wide range of operating temperatures. For example, the fire control radars on today’s jet fighters are liquid cooled using PAO. Boyd has PAO compatible recirculating chillers for testing cold plates and heat exchangers that will use PAO in their final application. PAO has a thermal conductivity of 0.14 W/m°C (0.081 BTU/hr ft °F). Although dielectric fluids provide low risk liquid cooling for electronics, they generally have a much lower thermal conductivity than water and most water-based solutions.</p></div>
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				<div class="et_pb_text_inner"><h2>Selecting Your Heat Transfer Fluid</h2></div>
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				<span class="et_pb_image_wrap "><img decoding="async" width="566" height="300" src="https://www.boydcorp.com/wp-content/uploads/Resources/Blog/Selecting-Your-Heat-Transfer-Fluid-566x300-1.jpg" alt="Selecting Your Heat Transfer Fluid" title="" class="wp-image-14750" /></span>
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				<div class="et_pb_text_inner"><p>Water, deionized water, glycol/water solutions, and dielectric fluids such as fluorocarbons and PAO are the heat transfer fluids most commonly used in high performance liquid cooling applications. It’s important to select a heat transfer fluid that is compatible with your fluid path, offers corrosion protection or minimal risk of corrosion, and meets your application’s specific requirements. With the right chemistry, your heat transfer fluid can provide very effective cooling for your liquid cooling loop.</p>
<p>For more information on <a href="https://www.boydcorp.com/thermal/liquid-cooling-systems.html">liquid cooling technologies</a> and the proper working fluid to use in your system, <a href="https://www.boydcorp.com/contact-us.html">contact us</a>.</p></div>
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			</div><p>The post <a href="https://www.boydcorp.com/blog/best-heat-transfer-fluids.html">The Best Heat Transfer Fluids for Liquid Cooling</a> appeared first on <a href="https://www.boydcorp.com">Boyd | Trusted Innovation</a>.</p>
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		<title>Reducing Contact Thermal Resistance</title>
		<link>https://www.boydcorp.com/blog/reducing-contact-thermal-resistance.html</link>
		
		<dc:creator><![CDATA[Boyd Blog]]></dc:creator>
		<pubDate>Wed, 13 May 2020 12:53:00 +0000</pubDate>
				<category><![CDATA[Blog]]></category>
		<category><![CDATA[Conduction Cooling]]></category>
		<category><![CDATA[Thermal]]></category>
		<category><![CDATA[heat transfer]]></category>
		<category><![CDATA[thermal interface material]]></category>
		<category><![CDATA[thermal management]]></category>
		<category><![CDATA[thermal management solutions]]></category>
		<guid isPermaLink="false">https://staging.boydcorp.com/reducing-contact-thermal-resistance/</guid>

					<description><![CDATA[<p>The post <a href="https://www.boydcorp.com/blog/reducing-contact-thermal-resistance.html">Reducing Contact Thermal Resistance</a> appeared first on <a href="https://www.boydcorp.com">Boyd | Trusted Innovation</a>.</p>
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										<content:encoded><![CDATA[<div class="et_pb_section et_pb_section_1 et_section_regular" >
				
				
				
				
				
				
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				<div class="et_pb_text_inner"><h2>Improving Heat Transfer Between Surfaces and Overall Thermal Performance</h2>
<p>This thermal resistance can be expressed as Rja, where:</p>
<ul>
<li>Rja &#8211; Thermal resistance from the device junction to ambient air or water</li>
<li>Rjc &#8211; Thermal resistance from the device junction to the package case, determined by the electronic device manufacturer (designer has no direct influence)</li>
<li>Rcs &#8211; Thermal resistance from the package case to the heat sink or cold plate, determined by the size and quality of the contact areas between the electronic device and the heat sink or cold plate, the materials used, and contact pressure</li>
<li>Rsa &#8211; Thermal resistance from the heat sink or cold plate to ambient air or water, determined by the heat sink or cold plate design (material and geometry)</li>
</ul>
<p>Therefore, one way to reduce Rja is to reduce Rcs, the contact resistance between the electronic device case and ambient-cooled, finned heat sinks or liquid-cooled cold plates. There are several factors that impact Rcs, including surface flatness, surface roughness, contact force or clamping pressure, surface cleanliness, and interface materials.<a class="eb-image-viewport"><img decoding="async" src="data:image/gif;base64,R0lGODlhAQABAIAAAAAAAP///yH5BAEAAAAALAAAAAABAAEAAAIBRAA7" /></a></p></div>
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				<div class="et_pb_text_inner"><h3>Surface Flatness and Surface Roughness<a class="eb-image-viewport"><img decoding="async" src="data:image/gif;base64,R0lGODlhAQABAIAAAAAAAP///yH5BAEAAAAALAAAAAABAAEAAAIBRAA7" /></a></h3></div>
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				<div class="et_pb_text_inner"><p>Surface flatness can be understood as widely spaced surface irregularities or &#8220;waviness&#8221; of a surface. Surface roughness is the submicron scale irregularities of a surface, usually as a result of machining, usage, and/or wear.</p>
<p>The contact between two imperfect surfaces will result in air gaps between them. (See Fig. 1.) Most contact areas consist of more than 90% air voids, which represent a significant resistance to heat transfer since air is not a very effective thermal conductor. Table 1 shows typical surface roughness values for different manufacturing processes.<a class="eb-image-viewport"><img decoding="async" src="data:image/gif;base64,R0lGODlhAQABAIAAAAAAAP///yH5BAEAAAAALAAAAAABAAEAAAIBRAA7" /></a></p></div>
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				<span class="et_pb_image_wrap "><img decoding="async" width="320" height="300" src="https://www.boydcorp.com/wp-content/uploads/2020/11/Surface-Flatness-and-Roughness-Diagram.jpg" alt="Figure 2: Surface-Flatness-and-Roughness-Diagram" title="" class="wp-image-1308" /></span>
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				<div class="et_pb_text_inner"><h4>Table 1:</h4></div>
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<table id="tablepress-48" class="tablepress tablepress-id-48">
<thead>
<tr class="row-1">
	<th class="column-1">Process</th><th class="column-2">Units in µm</th><th class="column-3">Units in µin</th>
</tr>
</thead>
<tbody class="row-striping row-hover">
<tr class="row-2">
	<td class="column-1">Polishing</td><td class="column-2">0.1 – 0.4</td><td class="column-3">4 – 16</td>
</tr>
<tr class="row-3">
	<td class="column-1">Grinding</td><td class="column-2">0.1 – 1.6</td><td class="column-3">4 – 64</td>
</tr>
<tr class="row-4">
	<td class="column-1">Laser Cutting</td><td class="column-2">0.8 – 6.3</td><td class="column-3">32 – 252</td>
</tr>
<tr class="row-5">
	<td class="column-1">Die Casting</td><td class="column-2">0.8 – 1.6</td><td class="column-3">32 – 64</td>
</tr>
<tr class="row-6">
	<td class="column-1">Machining</td><td class="column-2">0.8 – 1.6</td><td class="column-3">32 – 64</td>
</tr>
<tr class="row-7">
	<td class="column-1">Extrusion</td><td class="column-2">0.8 -3.2</td><td class="column-3">32 – 128</td>
</tr>
<tr class="row-8">
	<td class="column-1">Drilling</td><td class="column-2">1.6 – 6.3</td><td class="column-3">64 – 252</td>
</tr>
</tbody>
</table>
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				<div class="et_pb_text_inner"><p>A mounting surface flatness of 0.001 in/in is generally required for satisfactory contact between the electronic device and the heat sink or cold plate. The surface roughness should be equivalent to that of the electronic device, where 32-64 µin is usually adequate. Finer finishes add unnecessary cost with little or no improvement in thermal performance. Surface flatness is typically much more critical than surface finish in achieving a good thermal interface.<a class="eb-image-viewport"><img decoding="async" src="data:image/gif;base64,R0lGODlhAQABAIAAAAAAAP///yH5BAEAAAAALAAAAAABAAEAAAIBRAA7" /></a></p></div>
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				<div class="et_pb_text_inner"><h3>Contact Force</h3>
Another very important factor in minimizing contact thermal resistance is contact force, or the force with which the electronic device is pushed against the heat sink or cold plate. Electronic device and heat sink surfaces will never be perfectly flat. Consequently, there will always be air gaps in between. However, as the contact force pushing the two surfaces together increases so does the number of contact points between the two surfaces, resulting in a lower case-to-sink thermal resistance, Rcs. This relationship between force and thermal resistance does not follow a linear curve. As contact force is increased, contact thermal resistance will decrease until a point where it will show diminishing returns in thermal resistance reduction and maximum force the package can handle is approached. The electronic device manufacturer should be contacted for recommended contact forces.
<h3>Surface Cleanliness</h3>
Mounting surface cleanliness is also important in minimizing contact thermal resistance. Mounting surfaces should be kept free of all foreign material, such as dirt, oil, oxides, and films. Since most heat sinks and cold plates are stored after machining, a cleaning operation is recommended prior to mounting the device. A satisfactory cleaning technique is to lightly polish the mounting surface with 3M Scotch Brite® No.000 fine steel wool, followed by a semiconductor cleaning solvent wipe.
<h3>Thermal Interface Material</h3>
Finally, in order to further improve Rcs, an appropriate Thermal Interface Material (TIM) should be used to fill air gaps between the two surfaces. There are a number of technologies that can be used, including thermal greases and thermally conductive compounds, elastomers, adhesive tapes, etc., each with their own characteristics (operating temperatures, ease of application, curing time, pressure requirements, etc.) that can make them more or less desirable depending on the application. Contact Boyd to consult on how to select the appropriate TIM for your application. Table 2 shows typical thermal resistance and thermal conductivity values for these TIMs.</div>
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<table id="tablepress-49" class="tablepress tablepress-id-49">
<thead>
<tr class="row-1">
	<th class="column-1">Interface</th><th class="column-2">Thickness (in.)</th><th class="column-3">Thermal Conductivity, k(W/m-K)</th><th class="column-4">Rcs(°C/W)</th>
</tr>
</thead>
<tbody class="row-striping row-hover">
<tr class="row-2">
	<td class="column-1">Dry Joint</td><td class="column-2">N/A</td><td class="column-3">N/A</td><td class="column-4">2.9</td>
</tr>
<tr class="row-3">
	<td class="column-1">Thermal Grease</td><td class="column-2">0.003</td><td class="column-3">0.7</td><td class="column-4">0.9</td>
</tr>
<tr class="row-4">
	<td class="column-1">Thermal Compound</td><td class="column-2">0.005</td><td class="column-3">1.2</td><td class="column-4">0.8</td>
</tr>
<tr class="row-5">
	<td class="column-1">Elastomer</td><td class="column-2">0.010</td><td class="column-3">5.0</td><td class="column-4">1.8</td>
</tr>
<tr class="row-6">
	<td class="column-1">Adhesive Tape</td><td class="column-2">0.009</td><td class="column-3">0.7</td><td class="column-4">2.7</td>
</tr>
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				<div class="et_pb_text_inner"><h3>Contact Thermal Resistance Factors Review</h3>
<p>Contact conditions encompass a number of areas including surface flatness, surface roughness, surface cleanliness, contact pressure, and interface materials. There are many technologies and techniques available for optimizing the thermal path from the electronic device junction to the heat sink. It&#8217;s important to minimize the thermal resistance in order to maintain the electronic device temperature below its maximum rated value and increase the end product reliability.</p></div>
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			</div><p>The post <a href="https://www.boydcorp.com/blog/reducing-contact-thermal-resistance.html">Reducing Contact Thermal Resistance</a> appeared first on <a href="https://www.boydcorp.com">Boyd | Trusted Innovation</a>.</p>
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		<title>The Basics of Heat Transfer</title>
		<link>https://www.boydcorp.com/blog/thermal-management-heat-transfer-basics.html</link>
		
		<dc:creator><![CDATA[Boyd Blog]]></dc:creator>
		<pubDate>Mon, 10 Jun 2019 12:53:00 +0000</pubDate>
				<category><![CDATA[Blog]]></category>
		<category><![CDATA[Thermal]]></category>
		<category><![CDATA[heat dissipation]]></category>
		<category><![CDATA[heat transfer]]></category>
		<category><![CDATA[radiation]]></category>
		<category><![CDATA[thermal management]]></category>
		<guid isPermaLink="false">https://staging.boydcorp.com/thermal-management-heat-transfer-basics/</guid>

					<description><![CDATA[<p>The post <a href="https://www.boydcorp.com/blog/thermal-management-heat-transfer-basics.html">The Basics of Heat Transfer</a> appeared first on <a href="https://www.boydcorp.com">Boyd | Trusted Innovation</a>.</p>
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				<div class="et_pb_text_inner"><h2>Heat Spreading</h2></div>
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				<div class="et_pb_text_inner"><p>Heat spreaders offer cost-effective, reliable high thermal conductivity and efficacy with almost no moving parts.</p>
<p>A heat spreader is an effective solution for dealing with heat sources that have a high heat-flux density (high heat flow per unit area) and where the secondary heat exchanger in itself is not an effective method of dispersing heat (due to space limitations, energy use, cost, etc.). Heat spreaders can allow designers to use an air-cooled, rather than liquid-cooled, secondary heat exchanger.</p></div>
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				<div class="et_pb_text_inner"><p>Most heat spreaders are copper plates that function as heat exchangers. Heat spreaders transfer heat between its source and (generally) a secondary heat exchanger. The heat &#8220;spreads&#8221; from the heat source through the heat spreader, thus moving from a smaller to a larger cross sectional area (the secondary heat exchanger). While the heat flow is the same in the heat spreader as in the secondary heat exchanger, the heat flux density is reduced, making it easier to dissipate the heat via air cooling. The lower heat flux density also allows the secondary heat exchanger to be made of less expensive materials.</p></div>
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				<span class="et_pb_image_wrap "><img decoding="async" width="737" height="415" src="https://www.boydcorp.com/wp-content/uploads/2019/06/Heat-Spreading-Basics-of-Heat-Transfer-737x415.jpg" alt="Heat-Spreading-Basics-of-Heat-Transfer" title="" class="wp-image-1353" /></span>
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				<div class="et_pb_text_inner"><p>Boyd offers a variety of heat spreading technologies that provide significant improvement in solution effective thermal conductivities. These heat spreading technologies include:</p>
<ul>
<li>Advanced Solid Conduction (k-Core®/ Graphite Technologies)</li>
<li>Embedded Heat Pipe Cold Plates</li>
<li>Vapor Chamber Assemblies</li>
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				<div class="et_pb_text_inner"><h2>Heat Transfer</h2></div>
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				<div class="et_pb_text_inner"><h3>Heat Pipes</h3>
Heat pipes can be used to move heat over distances ranges from a few inches (&gt;50mm) to greater than 3 feet (&gt; 1 meter). In a heat pipe, heat from a heat source enters the evaporator end of the heat pipe, causing the working fluid to change phase from liquid to vapor. The vapor travels through the vapor space within the heat pipe to the other end, the condenser end, where a heat sink or other secondary heat dissipation device removes the heat energy. The release of heat in the condenser end causes the vapor to condense back to liquid which is absorbed into a capillary wick structure. The capillary wick structures incorporated into the internal walls of a heat pipe allow the liquid condensate inside the heat pipe to return from the condenser section of the heat pipe to the evaporator section via capillary action.

The heat-moving efficiency of this thermal solution is determined by factors such as wick, working fluid, diameter, length, bending, flattening and orientation.</div>
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				<span class="et_pb_image_wrap "><img decoding="async" width="737" height="415" src="https://www.boydcorp.com/wp-content/uploads/2019/06/Heat-Transfer-Basics-of-Heat-Transfer-737x415.jpg" alt="Heat-Transfer-Basics-of-Heat-Transfer" title="" class="wp-image-1354" /></span>
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				<div class="et_pb_text_inner"><p>The four common, commercially produced heat pipe wick structures are grooves in the internal tube wall, wire or screen mesh, sintered powder metal and fiber/spring. Different wicks have varying capillary limits (the capillary pumping rate at which the working fluid travels from condenser to evaporator).</p></div>
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				<div class="et_pb_text_inner"><h4>Loop Heat Pipes</h4>
<p>A loop heat pipe (LHP) is also a two-phase heat transfer device that uses capillary action to remove heat from a source and passively move it to a condenser or radiator. LHPs are similar to heat pipes but have the advantage of being able to provide reliable operation over long distance (up to 75 meters) and the ability to operate against gravity (high g environments).</p>
<p>In a loop heat pipe, the wick structure is only in the evaporator and the vaporized fluid is separated from the liquid and travels in a loop through the condenser back to the evaporator. Boyd has developed and manufactured different designs of LHPs ranging from powerful, large size LHPs (&gt;2000W) to miniature LHPs (&lt;100W) that have been successfully employed in a wide range of aerospace and ground based applications.</p></div>
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				<div class="et_pb_text_inner"><h2>Working Fluids, Operating Temperature Ranges, Orientation and Forming</h2>
<p>The type of working fluid also influences heat pipe performance. A heat pipe or loop heat pipe only functions when the working fluid temperature is above its freezing point. When the temperature is above the vapor condensation point of the working fluid, the vapor will not condense back to liquid phase, and no fluid circulation – and no cooling – occurs. Working Fluid selection is based on the operating temperature range of the application.<br />Boyd has designed and developed heat pipes and loop heat pipes for operating temperature ranges from Cryogenic (&lt;-250°C) to High Temperature (&gt;2000°C). Water is the most common working fluid due to its favorable thermal properties and operating temperature range of 5°C to 250°C.</p>
<p>Boyd has designed, developed and manufactured heat pipes using over 27 different working fluids.</p>
<p>The orientation of a heat pipe relative to gravity, combined with its wick structure, also plays an important role in its performance. For example, the groove wick has the lowest capillary limit but works best under gravity-assisted conditions, where the evaporator is located below the condenser. Loop heat pipes are less sensitive to orientation and rely on a high capillary pumping wick in the evaporator to drive performance.</p>
<p>Heat pipes can be formed (flattened or bent) for integration into an assembly. If a heat pipe is flattened or bent, it will reduce the maximum amount of heat that can be transported. Avoiding this limitation is a design consideration.</p>
<h2>Heat Pipe Applications</h2>
<p>For moving heat in industrial, electronic, aerospace and other applications, heat pipes and loop heat pipes are generally integrated into a thermal subsystem to transport heat from the heat source to remote areas. Heat pipes are effective in carrying heat away from heat sources and heat-sensitive components to a finned array or a heat sink in another location.</p>
<p>A high-capacity power electronics cooler is an example of a thermal solution where space is often insufficient for mounting a finned heat sink directly adjacent to the heat source. Instead, high-capacity heat pipes move the heat to the finned array, which dissipates heat energy using forced convection. Hundreds of watts can be dissipated this way.</p>
<h2>Benefits of Heat Pipes and Loop Heat Pipes</h2>
<p>The integration of heat pipes and loop heat pipes into a thermal solution delivers many benefits, including.</p>
<ul>
<li>High effective thermal conductivity (&gt;5000 W/m•K)</li>
<li>Long distance heat transport</li>
<li>High reliability</li>
<li>No moving parts</li>
<li>Cost-effective</li>
<li>Passive — do not require moving parts and other similar potential maintenance challenges</li>
</ul>
<p>In addition, heat pipes and loop heat pipes can be designed for a variety of external environmental factors such as mechanical shock, vibration, force impact, thermal shock/cycling, and corrosive environment that can affect heat pipe life.</p>
<h3>Dispersing Heat</h3>
<p>Using thermal solution technologies from Boyd such as heat sinks, heat pipes, vapor chambers, loop heat pipes, k-Core®, liquid cold plates, and heat exchangers, designers can choose to dissipate waste heat to air (natural or forced convection), to liquid (water, water/glycol, PAO), or radiate to space.</p>
<h3>Dissipating Heat to Air</h3>
<p>In many applications, the preferred method of thermal management is convection cooling to air, especially in electronics cooling applications. With Boyd&#8217;s heat sink, heat pipe assemblies, and heat spreader technologies, waste heat is typically absorbed from a heat generating device (e.g., an electrical component within an electronics system — i.e. computers and data centers) and then moved or spread for dissipation into the ambient air through either natural or forced (using a fan air mover). Thermal technologies from Boyd such as remote heat pipe assemblies and vapor chambers allow the designer to move heat from high heat flux components to a location with a larger surface area (typically plate fins or folded fins) and lower heat flux for dissipation into the ambient air.</p>
<h3>Dissipating Heat to Liquid</h3>
<p>Applications with large heat loads such as military radars or power electronics often require waste heat to be dissipated into the liquid coolants (water, water/glycol, PAO) of a secondary system for ultimate heat dissipation. Boyd&#8217;s heat pipe cold plates and liquid cold plates allow designers to move heat from a heat generating device into a coolant being circulated from a secondary system.</p>
<h3>Dissipating Heat through Radiation</h3>
<p>As satellites are packaged with more electronics, the challenge of rejecting heat through the limited surface area becomes greater. Boyd&#8217;s low temperature, axially grooved heat pipes (ammonia/aluminum, ethane/aluminum) and loop heat pipe technology make it possible to reject heat through radiator panels that are stored for launch, then deployed from the satellite when the satellite achieves orbit. Our low temperature axially grooved heat pipes spread heat out from the satellite electronics to the radiator panels, dissipating waste heat to space. And our loop heat pipe technology is capable of transporting and rejecting heat loads from hundreds of W to greater than 2,000 W.</p></div>
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			</div><p>The post <a href="https://www.boydcorp.com/blog/thermal-management-heat-transfer-basics.html">The Basics of Heat Transfer</a> appeared first on <a href="https://www.boydcorp.com">Boyd | Trusted Innovation</a>.</p>
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		<title>Fundamentals of Heat Transfer</title>
		<link>https://www.boydcorp.com/blog/heat-transfer-fundamentals.html</link>
		
		<dc:creator><![CDATA[Boyd Blog]]></dc:creator>
		<pubDate>Tue, 25 Sep 2018 12:53:00 +0000</pubDate>
				<category><![CDATA[Blog]]></category>
		<category><![CDATA[Thermal]]></category>
		<category><![CDATA[forced convection]]></category>
		<category><![CDATA[heat transfer]]></category>
		<category><![CDATA[natural convection]]></category>
		<category><![CDATA[radiation]]></category>
		<category><![CDATA[thermal management]]></category>
		<guid isPermaLink="false">https://staging.boydcorp.com/heat-transfer-fundamentals/</guid>

					<description><![CDATA[<p>The post <a href="https://www.boydcorp.com/blog/heat-transfer-fundamentals.html">Fundamentals of Heat Transfer</a> appeared first on <a href="https://www.boydcorp.com">Boyd | Trusted Innovation</a>.</p>
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<p><span data-redactor-tag="span" data-verified="redactor" data-redactor-style="font-size: 18px" style="font-size: 18px;">The following is a brief overview of some fundamental heat transfer concepts. To learn more, the reader is encouraged to review the source publications and cited websites<span class="redactor-invisible-space"></span><span class="redactor-invisible-space"></span></span></p>
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<h2 style="font-family: Tahoma;"><span data-redactor-tag="span" data-verified="redactor" data-redactor-style="color: #e1523d" style="color: #e1523d;"><span data-redactor-tag="span" data-verified="redactor" data-redactor-style="font-size: 30px; color: #b6411a;  font-family: Tahoma" style="font-size: 30px; color: #b6411a; font-family: Tahoma;"></span><span data-redactor-tag="span" data-verified="redactor" data-redactor-style="font-size: 30px; font-family: Tahoma;  color: #b6411a; font-family: Tahoma" style="font-size: 30px; font-family: Tahoma;"><span data-redactor-tag="span" data-verified="redactor" data-redactor-style="color: #b6411a" style="color: #b6411a;"><span data-redactor-tag="span" data-verified="redactor" data-redactor-style="font-family: Tahoma" style="font-family: Tahoma;">Introduction to Thermodynamics<span class="redactor-invisible-space"></span><span class="redactor-invisible-space"></span><span class="redactor-invisible-space"></span></span></span></span></span></h2>
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<h2 style="font-family: Tahoma;"><span data-redactor-tag="span" data-verified="redactor" data-redactor-style="color: #e1523d" style="color: #e1523d;"><span data-redactor-tag="span" data-verified="redactor" data-redactor-style="font-size: 30px; color: #b6411a;  font-family: Tahoma" style="font-size: 30px; color: #b6411a; font-family: Tahoma;"></span><span data-redactor-tag="span" data-verified="redactor" data-redactor-style="font-size: 30px; font-family: Tahoma;  color: #b6411a; font-family: Tahoma" style="font-size: 30px; font-family: Tahoma;"><span data-redactor-tag="span" data-verified="redactor" data-redactor-style="color: #b6411a" style="color: #b6411a;"><span data-redactor-tag="span" data-verified="redactor" data-redactor-style="font-size: 26px" style="font-size: 26px;"><span data-redactor-tag="span" data-verified="redactor" data-redactor-style="font-family: Tahoma" style="font-family: Tahoma;"><span data-redactor-tag="span" data-verified="redactor" data-redactor-style="color: #003057" style="color: #003057;"><strong data-redactor-tag="strong">1st and 2nd Laws of Thermodynamics<span class="redactor-invisible-space"></span></strong><span class="redactor-invisible-space"></span></span></span></span><span class="redactor-invisible-space" style="text-decoration-line: line-through;"></span><span class="redactor-invisible-space" style="text-decoration-line: line-through;"></span><span class="redactor-invisible-space" style="text-decoration-line: line-through;"></span><span class="redactor-invisible-space" style="text-decoration-line: line-through;"></span><span class="redactor-invisible-space" style="text-decoration-line: line-through;"></span><span class="redactor-invisible-space" style="text-decoration-line: line-through;"></span><span class="redactor-invisible-space" style="text-decoration-line: line-through;"></span><span data-redactor-tag="span" data-verified="redactor" data-redactor-style="font-family: Tahoma" style="font-family: Tahoma;"><span class="redactor-invisible-space"></span></span></span></span></span></h2>
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<p>The 1st Law of Thermodynamics involves the conservation of energy. It states that &#8211; within a closed system where no other energy material can enter or leave &#8211; energy can neither be created nor destroyed.<sup data-redactor-tag="sup">1, 2</sup> Although energy cannot be created or destroyed, it can be transferred to work as other forms of energy.</p>
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<p>Transferring heat energy is subject to the 2nd Law of Thermodynamics.<sup data-redactor-tag="sup">3</sup> The 2nd Law (again applying to a closed system) says that &#8211; for a spontaneous process &#8211; there is a net increase in entropy<sup data-redactor-tag="sup">4</sup> (i.e., a measure of the disorder that exists in a system<sup data-redactor-tag="sup">5</sup>).</p>
<p>&nbsp;</p>
<p>Three alternate but equivalent ways to describe the 2nd Law are:</p>
<p>&nbsp;</p>
<p>Heat flows spontaneously from a hot body to a cool one. (Example: A hot microprocessor or laser diode is cooled by flow of heat into heat sink or cold plate.)</p>
<p>&nbsp;</p>
<p>It is impossible to convert heat completely into useful work. (Example: In a combustion engine, a certain heat component must always be exhausted without performing work.)</p>
<p>&nbsp;</p>
<p>Every isolated system becomes disordered in time. (Example: In conduction when hot and cold bodies first contact each other, the system is somewhat ordered. Hotter molecules move faster than cooler molecules. But, once the entire system attains a uniform temperature, this order is lost.)</p>
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<p>Expressed in mathematical terms, any of the above statements imply the other two.<sup data-redactor-tag="sup">6</sup></p>
<p><sup data-redactor-tag="sup"> </sup></p>
<p>The 1st and 2nd Laws of Thermodynamics govern the various modes of heat transfer: conduction, convection and radiation.</p>
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<h2 style="font-family: Tahoma;"><span data-redactor-tag="span" data-verified="redactor" data-redactor-style="color: #e1523d" style="color: #e1523d;"><span data-redactor-tag="span" data-verified="redactor" data-redactor-style="font-size: 30px; color: #b6411a;  font-family: Tahoma" style="font-size: 30px; color: #b6411a; font-family: Tahoma;"></span><span data-redactor-tag="span" data-verified="redactor" data-redactor-style="font-size: 30px; font-family: Tahoma;  color: #b6411a; font-family: Tahoma" style="font-size: 30px; font-family: Tahoma;"><span data-redactor-tag="span" data-verified="redactor" data-redactor-style="color: #b6411a" style="color: #b6411a;"><span data-redactor-tag="span" data-verified="redactor" data-redactor-style="font-family: Tahoma" style="font-family: Tahoma;">Modes of Heat Transfer<span class="redactor-invisible-space"></span><span class="redactor-invisible-space"></span><span class="redactor-invisible-space"></span></span></span></span></span></h2>
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<p><span data-redactor-tag="span" data-verified="redactor" data-redactor-style="font-size: 18px" style="font-size: 18px;">In conduction, heat flows from a higher temperature region to regions of lower temperature. This occurs within solid, liquid, or gaseous mediums or between different mediums that make direct physical contact with each other.<sup data-redactor-tag="sup">7</sup> &#8220;The transfer of the energy of motion between adjacent molecules conducts the heat. In a gas, the &#8216;hotter&#8217; molecules, have greater energy and motions, and impart energy to adjacent molecules at lower energy levels. This type of transfer occurs to some extent in all solids, gases or liquids in which a temperature gradient exists. In conduction, energy can also be transferred by &#8220;free&#8221; electrons, which is important in metallic solids.&#8221;<sup data-redactor-tag="sup">8</sup> Examples of conduction are heat transfer through the surfaces of a cold plate or through the walls of a refrigerator.<span class="redactor-invisible-space"></span><span class="redactor-invisible-space"></span><span class="redactor-invisible-space"></span><span class="redactor-invisible-space"></span></span></p>
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<p><span data-redactor-tag="span" data-verified="redactor" data-redactor-style="font-size: 18px" style="font-size: 18px;">In convection, the combined action of heat conduction, energy storage, and mixing motion serve to transport energy. &#8220;Convection is most important as the mechanism of energy transfer between a solid surface and a liquid or a gas.&#8221;<sup data-redactor-tag="sup">9</sup> &#8220;In forced-convection heat transfer, a pump, fan, or other mechanism forces a fluid to flow past a solid surface. In natural or free convection, warmer or cooler fluid next to the solid surface causes a circulation because of density differences resulting from the temperature differences in the fluid.&#8221;<sup data-redactor-tag="sup">10</sup> An example of free convection is the loss of heat into ambient air via the fins of a heat exchanger. If a fan is used to circulate the air over the heat exchanger fins, this becomes an example of forced convection.<span class="redactor-invisible-space"></span><span class="redactor-invisible-space"></span><span class="redactor-invisible-space"></span><span class="redactor-invisible-space"></span><span class="redactor-invisible-space"></span></span></p>
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<p>In radiation, heat flows from a higher temperature body to a lower temperature body when the bodies are separated in space, even across a vacuum.<sup data-redactor-tag="sup">11</sup> &#8220;The same laws that govern the transfer of light, also govern the transfer of heat. Solids and liquids tend to absorb the radiation being transferred through it, hence radiation is important mainly in transfer through space or gases.&#8221;<sup data-redactor-tag="sup">12</sup></p>
<p><sup data-redactor-tag="sup"> </sup></p>
<p>Examples of radiation include the transfer of heat from the sun to the earth, and from a quartz lamp to a cool object that requires warming.</p>
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<h2 style="font-family: Tahoma;"><span data-redactor-tag="span" data-verified="redactor" data-redactor-style="color: #e1523d" style="color: #e1523d;"><span data-redactor-tag="span" data-verified="redactor" data-redactor-style="font-size: 30px; color: #b6411a;  font-family: Tahoma" style="font-size: 30px; color: #b6411a; font-family: Tahoma;"></span><span data-redactor-tag="span" data-verified="redactor" data-redactor-style="font-size: 30px; font-family: Tahoma;  color: #b6411a; font-family: Tahoma" style="font-size: 30px; font-family: Tahoma;"><span data-redactor-tag="span" data-verified="redactor" data-redactor-style="color: #b6411a" style="color: #b6411a;"><span data-redactor-tag="span" data-verified="redactor" data-redactor-style="font-family: Tahoma" style="font-family: Tahoma;">Mathematical Representation and Calculation of Heat Transfer<span class="redactor-invisible-space"></span><span class="redactor-invisible-space"></span><span class="redactor-invisible-space"></span><span class="redactor-invisible-space"></span></span></span></span></span></h2>
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<p>&#8220;The basic relation for heat transfer by conduction, proposed by the French scientist J.B.J. Fourier in 1822, states:</p>
<p>&nbsp;</p>
<p>The rate of heat flow by conduction in a material, qk , equals the product of the following three quantities:</p>
<p>&nbsp;</p>
<ul>
<li>k &#8211; Thermal conductivity of the material</li>
<li>A &#8211; Area of the section through which heat flows by conduction as measured perpendicularly to the direction of heat flow</li>
<li>dT/dx &#8211; Temperature gradient at the section, i.e., the rate of change of temperature T with respect to the difference in the direction of the heat flow x.</li>
</ul>
<p>Writing the heat conduction equation in mathematical form requires a sign convention; i.e., the direction of increasing distance x is the direction of positive heat flow. According to the second law of thermodynamics, heat will automatically flow from points of higher temperature to points of lower temperature. Thus, heat flow will be positive when the temperature gradient is negative. The basic equation for one-dimensional conduction in the steady state is: qk = -kA (dT/dx)&#8221;<sup data-redactor-tag="sup">13</sup>.</p>
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<p><span data-redactor-tag="span" data-verified="redactor" data-redactor-style="font-size: 18px" style="font-size: 18px;"><span class="redactor-invisible-space">Thermal conductivity is a measurement of the rate at which a given material will transfer heat.<sup data-redactor-tag="sup">14</sup> &#8220;The thermal conductivity of a substance is the quantity of heat in cal/sec passing through a body 1 cm thick with a cross section of 1 sq. cm when the temperature difference between the hot and cold sides of the body is 1 deg. C.&#8221;<sup data-redactor-tag="sup">15</sup> This intrinsic property is independent of the materials size, shape, or orientation.<span class="redactor-invisible-space"></span></span></span></p>
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<p><span data-redactor-tag="span" data-verified="redactor" data-redactor-style="font-size: 18px" style="font-size: 18px;"><span class="redactor-invisible-space">Thermal resistance is the inverse of thermal conductivity and indicates how a material inhibits the conduction of heat.<sup data-redactor-tag="sup">16</sup> Materials with a high thermal conductivity have a low thermal resistance and have poor heat insulation qualities (e.g., copper and aluminum). Conversely, materials with a low thermal conductivity have a high thermal resistance, and have good heat insulation qualities (e.g., fiberglass insulation and corkboard).<sup data-redactor-tag="sup">17</sup><span class="redactor-invisible-space"></span><span class="redactor-invisible-space"></span></span></span></p>
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<p><span data-redactor-tag="span" data-verified="redactor" data-redactor-style="font-size: 18px" style="font-size: 18px;"><span class="redactor-invisible-space">1. https://www.chemistry.ohio-state.edu/~woodward/ch121/ch5_law.html.</span></span></p>
<p>2. <a href="https://theory.uwinnipeg.ca/mod_tech/node78.html" target="_blank" rel="noopener noreferrer" style="box-sizing: border-box; font-family: helvetica, arial, 'hiragino sans gb', 宋体, 'sans-serif'; background-color: #ffffff; color: #428bca; text-decoration: none; margin: 0px; padding: 0px; font-size: 18px; font-style: normal; font-variant-ligatures: normal; font-variant-caps: normal; font-weight: 400; letter-spacing: normal; orphans: 2; text-align: start; text-indent: 0px; text-transform: none; white-space: normal; widows: 2; word-spacing: 0px; -webkit-text-stroke-width: 0px;">https://theory.uwinnipeg.ca/mod_tech/node78.html.</a></p>
<p>3. ibid.</p>
<p>4. http://learn.chem.vt.edu/tutorials/entropy/2ndlaw.html.</p>
<p>5. Microsoft Encarta World English Dictionary, St. Martin&#8217;s Press, 1999, Pp 596.</p>
<p>6. de Sorgo, Miksa, ibid.</p>
<p>7. de Sorgo, Miksa, &#8220;Understanding Phase Change Materials&#8221;, ElectronicsCooling Magazine, May. 2002</p>
<p>8. http://learn.chem.vt.edu/tutorials/entropy/2ndlaw.html.</p>
<p>9. Kreith, Frank, Principles of Heat Transfer, 2nd Edition, University of Colorado, International Textbook Co., Chapter 1, Pp 6.</p>
<p>10. Transport Processes and Unit Operations, 3rd Edition, Christie Geankopolis, University of Minn. Prentice Hall, Chapter 4, Pp 215.</p>
<p>11. Kreith, Frank, Principles of Heat Transfer, 2nd Edition, University of Colorado, International Textbook Co., Page 8.</p>
<p>12. Transport Processes and Unit Operations, 3rd Edition, Christie Geankopolis, University of Minn. Prentice Hall, Chapter 4, Pp 216.</p>
<p>13. Kreith, Frank, Principles of Heat Transfer, 2nd Edition, University of Colorado, International Textbook Co., Pp 7.</p>
<p>14. Transport Processes and Unit Operations, 3rd Edition, Christie Geankopolis, University of Minn. Prentice Hall, Chapter 4, Pp 216.</p>
<p>15. Kreith, Frank, Principles of Heat Transfer, 2nd Edition, University of Colorado, International Textbook Co., Pp 9.</p>
<p>16. Transport Processes and Unit Operations, 3rd Edition, Christie Geankopolis, University of Minn. Prentice Hall, Chapter 4, Pp 216.</p>
<p>17. <a href="http://theory.uwinnipeg.ca/mod_tech/node75.html" target="_blank" rel="noopener noreferrer" style="box-sizing: border-box; font-family: helvetica, arial, 'hiragino sans gb', 宋体, 'sans-serif'; background-color: #ffffff; color: #428bca; text-decoration: none; margin: 0px; padding: 0px; font-size: 18px; font-style: normal; font-variant-ligatures: normal; font-variant-caps: normal; font-weight: 400; letter-spacing: normal; orphans: 2; text-align: start; text-indent: 0px; text-transform: none; white-space: normal; widows: 2; word-spacing: 0px; -webkit-text-stroke-width: 0px;">http://theory.uwinnipeg.ca/mod_tech/node75.html.</a></p>
<p>18. http://www.lib.umich.edu/dentlib/dental_tables/thermcond.html.</p>
<p>19. http://www.xrefer.com/entry/619844.</p>
<p>20. <a href="http://theory.uwinnipeg.ca/mod_tech/node75.html" target="_blank" rel="noopener noreferrer" style="box-sizing: border-box; font-family: helvetica, arial, 'hiragino sans gb', 宋体, 'sans-serif'; background-color: #ffffff; color: #428bca; text-decoration: none; margin: 0px; padding: 0px; font-size: 18px; font-style: normal; font-variant-ligatures: normal; font-variant-caps: normal; font-weight: 400; letter-spacing: normal; orphans: 2; text-align: start; text-indent: 0px; text-transform: none; white-space: normal; widows: 2; word-spacing: 0px; -webkit-text-stroke-width: 0px;">http://theory.uwinnipeg.ca/mod_tech/node75.html.</a></p>
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			</div><p>The post <a href="https://www.boydcorp.com/blog/heat-transfer-fundamentals.html">Fundamentals of Heat Transfer</a> appeared first on <a href="https://www.boydcorp.com">Boyd | Trusted Innovation</a>.</p>
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		<title>How to Measure your Heat Load</title>
		<link>https://www.boydcorp.com/blog/measuring-your-heat-load.html</link>
		
		<dc:creator><![CDATA[Boyd Blog]]></dc:creator>
		<pubDate>Tue, 22 May 2018 12:53:00 +0000</pubDate>
				<category><![CDATA[Blog]]></category>
		<category><![CDATA[Thermal]]></category>
		<category><![CDATA[design engineering]]></category>
		<category><![CDATA[heat transfer]]></category>
		<category><![CDATA[thermal management]]></category>
		<guid isPermaLink="false">https://staging.boydcorp.com/measuring-your-heat-load/</guid>

					<description><![CDATA[<p>The post <a href="https://www.boydcorp.com/blog/measuring-your-heat-load.html">How to Measure your Heat Load</a> appeared first on <a href="https://www.boydcorp.com">Boyd | Trusted Innovation</a>.</p>
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				<div class="et_pb_text_inner"><p>The first step in selecting the right product for your cooling system application is to determine the heat load, or the amount of heat generated by your system. This article explains how to establish heat load for any <a href="https://www.boydcorp.com/thermal/liquid-cooling-systems.html">liquid cooling</a> application. The same process can be adapted for <a href="https://www.boydcorp.com/thermal/air-cooling.html">air cooling systems</a> as well.</p></div>
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				<div class="et_pb_text_inner"><h2>Rough Estimate for Heat Load</h2>
A quick and dirty method of estimating heat load is to assume that all electrical energy entering a process is converted to heat. From the 1st Law of Thermodynamics we know that the amount of energy exiting a system can never be greater than the amount of energy entering a system.  

The heat load can be conservatively estimated to be equal to the amount of electricity consumed if electricity is the only form of energy entering a system. </div>
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				<div class="et_pb_text_inner"><h2>Formula for Specific Heat</h2>
To determine heat load more accurately, use the heat transfer equation:

Q = m x Cp x ΔT where:
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<li>Q = heat load (W [BTU/hr])</li>
<li>m = mass flow rate (kg/s [lb/hr])</li>
<li>Cp = specific heat (J/g-K [BTU/lb °F])</li>
<li>ΔT = change in temperature (°C [°F])</li>
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				<div class="et_pb_text_inner"><h2>Test Setup for Calculating Heat Load</h2>
To determine Q using the above heat transfer equation, you will need to obtain the values m and ΔT experimentally. To measure these the temperature differential and mass flow rate values you will need the following equipment:  

Two (2x) Type “T” Thermocouples – Recommended accuracy: ± 0.2°F 

A Turbine Flow Meter – Recommended accuracy: ± 1% of Reading 

The thermocouples and flow meter can be used to measure fluid temperature change and flow rate of the cooling fluid when your system is at peak load operation (see Figure 1). Using the fluid’s specific heat (properties of commonly used fluids can be found in the Thermal Reference Guide in our Technical Library) and the above equation, heat load can be computed. </div>
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				<span class="et_pb_image_wrap "><img decoding="async" width="332" height="261" src="https://www.boydcorp.com/wp-content/uploads/2018/05/Heat-Load-Test-Setup-Thermocouples.jpg" alt="" title="Heat-Load-Test-Setup-Thermocouples" class="wp-image-1371" /></span>
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				<div class="et_pb_text_inner"><h2>What Are Thermocouples?</h2>
<p>Thermocouples are a sensor built from two dissimilar metals that generate an electrical charge based on the temperature at the joint between those two materials. Thermocouples are a crucial element in <a href="https://www.boydcorp.com/applications/test-systems.html">thermal testing</a>.</p>
<p>Accurate measurements rely on placing the thermocouple junction as close to the point under test. If a material is in the way, thermal resistance and thickness can also help determine the temperature at a specific point but decrease the overall accuracy of your measurement.</p></div>
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				<div class="et_pb_text_inner"><h3>Thermocouples Measurement Accuracy</h3>
The accuracy of the thermocouples and flow meter is particularly important, as a small decrease in accuracy can cause a significant error percentage. For example: if the temperature rise is 10 °C and the thermocouples are accurate to ± 0.5 °C, the temperature rise measurement could be off by as much as 1 °C, or 10%. This means that the overall heat load calculation cannot be more accurate than that ±10%. If the temperature rise is less than 10 °C, the ± 0.5 °C becomes an even higher error percentage. When the temperature error is given in °F or °C, the error percentage can be calculated by multiplying the thermocouple accuracy by two, then dividing by the change in temperature, and multiplying by one hundred.</div>
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				<div class="et_pb_text_inner"><h3>Thermocouple Calibration</h3>
We recommend calibrating the two thermocouples prior to recording measurements. If this isn’t possible, the accuracy of one thermocouple can be compared to the other. To do this, run a fluid stream through the thermocouples with no heat load. If the temperatures are the same, the exact temperature rise at peak operation can be used. Otherwise, account for the temperature difference of the two thermocouples under no heat load when conducting measurements at peak load operation. For thermocouples measuring different temperatures, subtract the temperature difference with no heat load from the temperature difference with heat load applied.

For example: if the two thermocouples read 20.0 and 20.5°C when under no heat load, and 25.0 and 30.5°C with heat load applied, the change in temperature should be calculated to be (30.5 &#8211; 25.0) &#8211; (20.5 &#8211; 20.0), or 5.0°C.</div>
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				<div class="et_pb_text_inner"><h2>How to Measure Liquid Flow Rate Without a Flow Meter</h2>
<p>If a flow meter is not available, measure the constant flow rate of the system with a graduated container and a timer. Collect the fluid in the graduated container over a measured period. Divide the amount of fluid by the amount of time that has elapsed. A constant flow rate is essential when measuring the flow in this manner. The density of the fluid should be used to convert the volumetric flow rate to mass flow rate.</p>
<p>These methods of determining heat load are generic to any liquid cooling application and can be used when sizing a <a href="https://www.boydcorp.com/thermal/liquid-cooling-systems/coolant-distribution-unit-cdu.html">CDU</a>, <a href="https://www.boydcorp.com/thermal/liquid-cooling-systems/chillers.html">recirculating chiller</a>, <a href="https://www.boydcorp.com/thermal/liquid-cooling-systems/liquid-cold-plates.html">cold plate</a>, or <a href="https://www.boydcorp.com/thermal/liquid-cooling-systems/heat-exchangers.html">heat exchanger</a>.</p></div>
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				<div class="et_pb_text_inner"><h2>Now I Know my Heat Load, What Next?</h2>
<p>Once you’ve calculated the heat load of your system, you can start determining the amount of cooling you require. This piece of information combined with the amount of volume allowable for a cooling system will help thermal engineers select or develop a <a href="https://www.boydcorp.com/thermal/liquid-cooling-systems.html">liquid cooling system</a> that will meet your project needs.</p>
<p>Need help getting a pulse on your system? <a href="https://www.boydcorp.com/contact-us.html">Contact our engineering team</a> or learn more about our <a href="https://www.boydcorp.com/applications/test-systems.html">Testing Services</a>.</p></div>
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				<div class="et_pb_text_inner"><h2>Test Your Knowledge!</h2></div>
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			</div><p>The post <a href="https://www.boydcorp.com/blog/measuring-your-heat-load.html">How to Measure your Heat Load</a> appeared first on <a href="https://www.boydcorp.com">Boyd | Trusted Innovation</a>.</p>
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