{"id":1562,"date":"2016-03-09T18:10:13","date_gmt":"2016-03-09T18:10:13","guid":{"rendered":"http:\/\/machineryequipmentonline.com\/hydraulics-and-pneumatics\/?p=1562"},"modified":"2016-03-09T18:10:13","modified_gmt":"2016-03-09T18:10:13","slug":"energy-transfer-by-heatworkand-massheat-transfer","status":"publish","type":"post","link":"http:\/\/machineryequipmentonline.com\/hydraulics-and-pneumatics\/energy-transfer-by-heatworkand-massheat-transfer\/","title":{"rendered":"ENERGY TRANSFER BY HEAT,WORK,AND MASS:HEAT TRANSFER"},"content":{"rendered":"<div class=\"ngqyy6a0dcd57b0878\" ><script type=\"text\/javascript\">\n\tatOptions = {\n\t\t'key' : '61e5902552e2353963d8d2f1bd1f4a8f',\n\t\t'format' : 'iframe',\n\t\t'height' : 250,\n\t\t'width' : 300,\n\t\t'params' : {}\n\t};\n<\/script>\n<script type=\"text\/javascript\" src=\"\/\/www.highperformanceformat.com\/61e5902552e2353963d8d2f1bd1f4a8f\/invoke.js\"><\/script><\/div><style type=\"text\/css\">\r\n@media screen and (min-width: 1201px) {\r\n.ngqyy6a0dcd57b0878 {\r\ndisplay: block;\r\n}\r\n}\r\n@media screen and (min-width: 993px) and (max-width: 1200px) {\r\n.ngqyy6a0dcd57b0878 {\r\ndisplay: block;\r\n}\r\n}\r\n@media screen and (min-width: 769px) and (max-width: 992px) {\r\n.ngqyy6a0dcd57b0878 {\r\ndisplay: block;\r\n}\r\n}\r\n@media screen and (min-width: 768px) and (max-width: 768px) {\r\n.ngqyy6a0dcd57b0878 {\r\ndisplay: block;\r\n}\r\n}\r\n@media screen and (max-width: 767px) {\r\n.ngqyy6a0dcd57b0878 {\r\ndisplay: block;\r\n}\r\n}\r\n<\/style>\r\n<div align=\"justify\"><font size=\"5\">Energy can be transferred to or from a closed system (a fixed mass) in two distinct forms: <i>hea<\/i><i>t <\/i>and <i>work<\/i><i>. <\/i>For control volumes, energy can also be transferred by mass. An energy transfer to or from a closed sys<\/font><font size=\"5\">tem is <i>hea<\/i><i>t <\/i>if it is caused by a temperature difference between the system and its surroundings. Otherwise it is <i>work<\/i><i>, <\/i>and it is caused by a force acting through a distance. We start this chapter with a discussion of energy transfer by <i>heat<\/i><i>. <\/i>We then introduce various forms of <i>work<\/i><i>, <\/i>with particular emphasis on the <i>moving boundary work <\/i>or <i>P dV work <\/i>commonly encountered in reciprocating devices such as automotive engines and compressors. We continue with the <i>flo<\/i><i>w work, <\/i>which is the work associated with forcing a fluid into or out of a control volume, and show that the combination of the internal energy and the flow work gives the property <i>enthalp<\/i><i>y<\/i><i>. <\/i>Then we discuss the <i>conserva- <\/i><i>tion of mass principle <\/i>and apply it to various systems. Finally, we show that <i>h <\/i>+ ke + pe represents the energy of a flowing fluid per unit of its mass.<\/font><\/div>\n<div align=\"justify\"><font size=\"5\"><\/font>&nbsp;<\/div>\n<div align=\"justify\"><font size=\"5\">&nbsp;<b>HE<\/b><b>A<\/b><b>T TRANSFER<\/b><\/font><\/div>\n<div align=\"justify\"><strong><font size=\"5\"><\/font><\/strong>&nbsp;<\/div>\n<div align=\"justify\"><font size=\"5\">Energy can cross the boundary of a closed system in two distinct forms: <i>heat <\/i>and <i>wor<\/i><i>k <\/i>(Fig. 4\u20131). It is important to distinguish between these two forms of energy. Therefore, they will be discussed first, to form a sound basis for the development of the principles of thermodynamics.<\/font><\/div>\n<p align=\"justify\"><font size=\"5\">We know from experience that a can of cold soda left on a table eventually warms up and that a hot baked potato on the same table cools down (Fig. 4\u20132). When a body is left in a medium that is at a different temperature, energy transfer takes place between the body and the surrounding medium until ther<\/font><font size=\"5\">mal equilibrium is established, that is, the body and the medium reach the <\/font><font size=\"5\">same temperature. The direction of energy transfer is always from the higher temperature body to the lower temperature one. Once the temperature equal- ity is established, energy transfer stops. In the processes described above, energy is said to be transferred in the form of heat.<\/font> <\/p>\n<p align=\"justify\"><font size=\"5\"><b>Hea<\/b><b>t <\/b>is defined as <i>the form of energy that is transferred between two sys- tems (or a system and its surroundings) by virtue of a temperature difference <\/i>(Fig. 4\u20133). That is, an energy interaction is heat only if it takes place because of a temperature difference. Then it follows that there cannot be any heat transfer between two systems that are at the same temperature.<\/font> <\/p>\n<p align=\"justify\"><font size=\"5\">In daily life, we frequently refer to the sensible and latent forms of internal energy as <i>heat<\/i>, and we talk about the heat content of bodies. In thermo- dynamics, however, we usually refer to those forms of energy as <i>thermal <\/i><i>ene<\/i><i>r<\/i><i>g<\/i><i>y <\/i>to prevent any confusion with <i>hea<\/i><i>t transfer<\/i>.<\/font> <\/p>\n<p align=\"justify\"><font size=\"5\">Several phrases in common use today\u2014such as heat flow, heat addition, heat rejection, heat absorption, heat removal, heat gain, heat loss, heat storage, heat generation, electrical heating, resistance heating, frictional heating, gas heating, heat of reaction, liberation of heat, specific heat, sensible heat, latent heat, waste heat, body heat, process heat, heat sink, and heat source\u2014are not consistent with the strict thermodynamic meaning of the term <i>heat<\/i>, which limits its use to the <i>transfe<\/i><i>r <\/i>of thermal energy during a process. However, these phrases are deeply rooted in our vocabulary, and they are used by both ordinary people and scientists without causing any misunderstanding since they are usually interpreted properly instead of being taken literally. (Besides, no acceptable alternatives exist for some of these phrases.) For example, the phrase <i>bod<\/i><i>y heat <\/i>is understood to mean <i>th<\/i><i>e thermal energy content <\/i>of a body. Likewise, <i>hea<\/i><i>t flow <\/i>is understood to mean <i>th<\/i><i>e transfer of thermal energy, <\/i>not<\/font> <\/p>\n<p align=\"justify\"><font size=\"5\"><a href=\"http:\/\/machineryequipmentonline.com\/hydraulics-and-pneumatics\/wp-content\/uploads\/2016\/03\/ENERGY-TRANSFER-BY-HEATWORKAND-MASS-0199.jpg\"><img decoding=\"async\" loading=\"lazy\" style=\"background-image: none; border-bottom: 0px; border-left: 0px; margin: 0px auto; padding-left: 0px; padding-right: 0px; display: block; float: none; border-top: 0px; border-right: 0px; padding-top: 0px\" title=\"ENERGY TRANSFER BY HEAT,WORK,AND MASS-0199\" border=\"0\" alt=\"ENERGY TRANSFER BY HEAT,WORK,AND MASS-0199\" src=\"http:\/\/machineryequipmentonline.com\/hydraulics-and-pneumatics\/wp-content\/uploads\/2016\/03\/ENERGY-TRANSFER-BY-HEATWORKAND-MASS-0199_thumb.jpg\" width=\"181\" height=\"364\"><\/a><a href=\"http:\/\/machineryequipmentonline.com\/hydraulics-and-pneumatics\/wp-content\/uploads\/2016\/03\/ENERGY-TRANSFER-BY-HEATWORKAND-MASS-0200.jpg\"><img decoding=\"async\" loading=\"lazy\" style=\"background-image: none; border-bottom: 0px; border-left: 0px; margin: 0px auto; padding-left: 0px; padding-right: 0px; display: block; float: none; border-top: 0px; border-right: 0px; padding-top: 0px\" title=\"ENERGY TRANSFER BY HEAT,WORK,AND MASS-0200\" border=\"0\" alt=\"ENERGY TRANSFER BY HEAT,WORK,AND MASS-0200\" src=\"http:\/\/machineryequipmentonline.com\/hydraulics-and-pneumatics\/wp-content\/uploads\/2016\/03\/ENERGY-TRANSFER-BY-HEATWORKAND-MASS-0200_thumb.jpg\" width=\"438\" height=\"173\"><\/a><\/font> <\/p>\n<p align=\"justify\"><font size=\"5\">the flow of a fluidlike substance called heat, although the latter incorrect interpretation, which is based on the caloric theory, is the origin of this phrase. Also, the transfer of heat into a system is frequently referred to as <i>hea<\/i><i>t addition <\/i>and the transfer of heat out of a system as <i>hea<\/i><i>t rejection<\/i>. Perhaps there <\/font><font size=\"5\">are thermodynamic reasons for being so reluctant to replace <i>heat <\/i>by <i>thermal energy<\/i>: It takes less time and energy to say, write, and comprehend <i>heat <\/i>than it does <i>thermal energy<\/i>.<\/font> <\/p>\n<p align=\"justify\"><font size=\"5\"><\/font> <\/p>\n<p align=\"justify\"><font size=\"5\">Heat is energy in transition. It is recognized only as it crosses the boundary of a system. Consider the hot baked potato one more time. The potato contains energy, but this energy is heat transfer only as it passes through the skin of the potato (the system boundary) to reach the air, as shown in Fig. 4\u20134. Once in the surroundings, the transferred heat becomes part of the internal energy of <\/font><font size=\"5\">the surroundings. Thus, in thermodynamics, the term <i>hea<\/i><i>t <\/i>simply means <i>heat transfe<\/i><i>r.<\/i><\/font><\/p>\n<p align=\"justify\"><font size=\"5\">A process during which there is no heat transfer is called an <b>adiabatic p<\/b><b>r<\/b><b>oces<\/b><b>s <\/b>(Fig. 4\u20135). The word <i>adiabati<\/i><i>c <\/i>comes from the Greek word <i>adiabatos<\/i><i>, <\/i>which means <i>no<\/i><i>t to be passed. <\/i>There are two ways a process can be adiabatic: Either the system is well insulated so that only a negligible amount of heat can pass through the boundary, or both the system and the surroundings are at the same temperature and therefore there is no driving force (temperature difference) for heat transfer. An adiabatic process should not be confused with an isothermal process. Even though there is no heat transfer during an adiabatic process, the energy content and thus the temperature of a system can still be changed by other means such as work.<\/font> <\/p>\n<p align=\"justify\"><font size=\"5\">As a form of energy, heat has energy units, kJ (or Btu) being the most common one. The amount of heat transferred during the process between two states (states 1 and 2) is denoted by <i>Q<\/i>12, or just <i>Q<\/i><i>. <\/i>Heat transfer <i>pe<\/i><i>r unit mass <\/i>of a system is denoted <i>q <\/i>and is determined from<\/font> <\/p><div class=\"hnhyd6a0dcd57b0a82\" ><script type=\"text\/javascript\">\n\tatOptions = {\n\t\t'key' : '0c1eb4c533eaedb7b996f49a5a4983a9',\n\t\t'format' : 'iframe',\n\t\t'height' : 300,\n\t\t'width' : 160,\n\t\t'params' : {}\n\t};\n<\/script>\n<script type=\"text\/javascript\" src=\"\/\/www.highperformanceformat.com\/0c1eb4c533eaedb7b996f49a5a4983a9\/invoke.js\"><\/script><\/div><style type=\"text\/css\">\r\n@media screen and (min-width: 1201px) {\r\n.hnhyd6a0dcd57b0a82 {\r\ndisplay: block;\r\n}\r\n}\r\n@media screen and (min-width: 993px) and (max-width: 1200px) {\r\n.hnhyd6a0dcd57b0a82 {\r\ndisplay: block;\r\n}\r\n}\r\n@media screen and (min-width: 769px) and (max-width: 992px) {\r\n.hnhyd6a0dcd57b0a82 {\r\ndisplay: block;\r\n}\r\n}\r\n@media screen and (min-width: 768px) and (max-width: 768px) {\r\n.hnhyd6a0dcd57b0a82 {\r\ndisplay: block;\r\n}\r\n}\r\n@media screen and (max-width: 767px) {\r\n.hnhyd6a0dcd57b0a82 {\r\ndisplay: block;\r\n}\r\n}\r\n<\/style>\r\n<div class=\"grisz6a0dcd57b097a\" ><script async src=\"https:\/\/pagead2.googlesyndication.com\/pagead\/js\/adsbygoogle.js?client=ca-pub-0778475562755157\"\n     crossorigin=\"anonymous\"><\/script>\n<!-- 300x600 hydraulics-and-pneumatics -->\n<ins class=\"adsbygoogle\"\n     style=\"display:inline-block;width:300px;height:600px\"\n     data-ad-client=\"ca-pub-0778475562755157\"\n     data-ad-slot=\"3735577695\"><\/ins>\n<script>\n     (adsbygoogle = window.adsbygoogle || []).push({});\n<\/script><\/div><style type=\"text\/css\">\r\n@media screen and (min-width: 1201px) {\r\n.grisz6a0dcd57b097a {\r\ndisplay: block;\r\n}\r\n}\r\n@media screen and (min-width: 993px) and (max-width: 1200px) {\r\n.grisz6a0dcd57b097a {\r\ndisplay: block;\r\n}\r\n}\r\n@media screen and (min-width: 769px) and (max-width: 992px) {\r\n.grisz6a0dcd57b097a {\r\ndisplay: block;\r\n}\r\n}\r\n@media screen and (min-width: 768px) and (max-width: 768px) {\r\n.grisz6a0dcd57b097a {\r\ndisplay: block;\r\n}\r\n}\r\n@media screen and (max-width: 767px) {\r\n.grisz6a0dcd57b097a {\r\ndisplay: block;\r\n}\r\n}\r\n<\/style>\r\n\n<p align=\"justify\"><font size=\"5\"><a href=\"http:\/\/machineryequipmentonline.com\/hydraulics-and-pneumatics\/wp-content\/uploads\/2016\/03\/ENERGY-TRANSFER-BY-HEATWORKAND-MASS-0201.jpg\"><img decoding=\"async\" loading=\"lazy\" style=\"background-image: none; border-bottom: 0px; border-left: 0px; margin: 0px auto; padding-left: 0px; padding-right: 0px; display: block; float: none; border-top: 0px; border-right: 0px; padding-top: 0px\" title=\"ENERGY TRANSFER BY HEAT,WORK,AND MASS-0201\" border=\"0\" alt=\"ENERGY TRANSFER BY HEAT,WORK,AND MASS-0201\" src=\"http:\/\/machineryequipmentonline.com\/hydraulics-and-pneumatics\/wp-content\/uploads\/2016\/03\/ENERGY-TRANSFER-BY-HEATWORKAND-MASS-0201_thumb.jpg\" width=\"227\" height=\"32\"><\/a><\/font> <\/p>\n<p align=\"justify\"><font size=\"5\">Sometimes it is desirable to know the <i>rate of heat transfer <\/i>(the amount of heat transferred per unit time) instead of the total heat transferred over some <\/font><font size=\"5\">time interval (Fig. 4\u20136). The heat transfer rate is denoted <i>\u00b7 <\/i>, where the over-<\/font><font size=\"5\">dot stands for the time derivative, or \u201cper unit time.\u2019\u2019 The heat transfer rate <i>Q <\/i>has the unit kJ\/s, which is equivalent to kW. When <i>\u00b7 <\/i>varies with time, the <\/font><font size=\"5\">amount of heat transfer during a process is determined by integrating <i>Q <\/i>over <\/font><font size=\"5\">the time interval of the process:<\/font> <\/p>\n<p align=\"justify\"><font size=\"5\"><a href=\"http:\/\/machineryequipmentonline.com\/hydraulics-and-pneumatics\/wp-content\/uploads\/2016\/03\/ENERGY-TRANSFER-BY-HEATWORKAND-MASS-0202.jpg\"><img decoding=\"async\" loading=\"lazy\" style=\"background-image: none; border-bottom: 0px; border-left: 0px; margin: 0px auto; padding-left: 0px; padding-right: 0px; display: block; float: none; border-top: 0px; border-right: 0px; padding-top: 0px\" title=\"ENERGY TRANSFER BY HEAT,WORK,AND MASS-0202\" border=\"0\" alt=\"ENERGY TRANSFER BY HEAT,WORK,AND MASS-0202\" src=\"http:\/\/machineryequipmentonline.com\/hydraulics-and-pneumatics\/wp-content\/uploads\/2016\/03\/ENERGY-TRANSFER-BY-HEATWORKAND-MASS-0202_thumb.jpg\" width=\"363\" height=\"109\"><\/a><a href=\"http:\/\/machineryequipmentonline.com\/hydraulics-and-pneumatics\/wp-content\/uploads\/2016\/03\/ENERGY-TRANSFER-BY-HEATWORKAND-MASS-0203.jpg\"><img decoding=\"async\" loading=\"lazy\" style=\"background-image: none; border-bottom: 0px; border-left: 0px; margin: 0px auto; padding-left: 0px; padding-right: 0px; display: block; float: none; border-top: 0px; border-right: 0px; padding-top: 0px\" title=\"ENERGY TRANSFER BY HEAT,WORK,AND MASS-0203\" border=\"0\" alt=\"ENERGY TRANSFER BY HEAT,WORK,AND MASS-0203\" src=\"http:\/\/machineryequipmentonline.com\/hydraulics-and-pneumatics\/wp-content\/uploads\/2016\/03\/ENERGY-TRANSFER-BY-HEATWORKAND-MASS-0203_thumb.jpg\" width=\"170\" height=\"484\"><\/a><\/font> <\/p>\n<p align=\"justify\"><font size=\"5\"><strong>Historical Background on Heat<\/strong><\/font> <\/p>\n<p align=\"justify\"><font size=\"5\">Heat has always been perceived to be something that produces in us a sensa<\/font><font size=\"5\">tion of warmth, and one would think that the nature of heat is one of the first <\/font><font size=\"5\">things understood by mankind. However, it was only in the middle of the nineteenth century that we had a true physical understanding of the nature of heat, thanks to the development at that time of the <b>kineti<\/b><b>c theory, <\/b>which treats <\/font><font size=\"5\">molecules as tiny balls that are in motion and thus possess kinetic energy. Heat is then defined as the energy associated with the random motion of atoms and molecules. Although it was suggested in the eighteenth and early nineteenth centuries that heat is the manifestation of motion at the molecular level (called the <i>liv<\/i><i>e force<\/i>), the prevailing view of heat until the middle of the nineteenth century was based on the caloric theory proposed by the French chemist Antoine Lavoisier (1744\u20131794) in 1789. The caloric theory asserts <\/font><font size=\"5\">In the early nineteenth century, heat was thought to be an invisible fluid called the <i>caloric <\/i>that flowed from warmer bodies to the cooler ones.<\/font> <\/p>\n<p align=\"justify\"><font size=\"5\">that heat is a fluidlike substance called the <b>calori<\/b><b>c <\/b>that is a massless, colorless, <\/font><font size=\"5\">odorless, and tasteless substance that can be poured from one body into an- other (Fig. 4\u20137). When caloric was added to a body, its temperature increased; and when caloric was removed from a body, its temperature decreased. When a body could not contain any more caloric, much the same way as when a glass of water could not dissolve any more salt or sugar, the body was said to be saturated with caloric. This interpretation gave rise to the terms <i>saturated liquid <\/i>and <i>saturate<\/i><i>d vapor <\/i>that are still in use today.<\/font> <\/p>\n<p align=\"justify\"><font size=\"5\">The caloric theory came under attack soon after its introduction. It maintained that heat is a substance that could not be created or destroyed. Yet it was known that heat can be generated indefinitely by rubbing one\u2019s hands together or rubbing two pieces of wood together. In 1798, the American Benjamin Thompson (Count Rumford) (1754\u20131814) showed in his papers that heat can be generated continuously through friction. The validity of the caloric theory was also challenged by several others. But it was the careful experiments of the Englishman James P. Joule (1818\u20131889) published in 1843 that finally convinced the skeptics that heat was not a substance after all, and thus put the caloric theory to rest. Although the caloric theory was totally abandoned in the middle of the nineteenth century, it contributed greatly to the development of thermodynamics and heat transfer.<\/font> <\/p>\n<p align=\"justify\"><font size=\"5\"><a href=\"http:\/\/machineryequipmentonline.com\/hydraulics-and-pneumatics\/wp-content\/uploads\/2016\/03\/ENERGY-TRANSFER-BY-HEATWORKAND-MASS-0204.jpg\"><img decoding=\"async\" loading=\"lazy\" style=\"background-image: none; border-bottom: 0px; border-left: 0px; margin: 0px auto; padding-left: 0px; padding-right: 0px; display: block; float: none; border-top: 0px; border-right: 0px; padding-top: 0px\" title=\"ENERGY TRANSFER BY HEAT,WORK,AND MASS-0204\" border=\"0\" alt=\"ENERGY TRANSFER BY HEAT,WORK,AND MASS-0204\" src=\"http:\/\/machineryequipmentonline.com\/hydraulics-and-pneumatics\/wp-content\/uploads\/2016\/03\/ENERGY-TRANSFER-BY-HEATWORKAND-MASS-0204_thumb.jpg\" width=\"176\" height=\"190\"><\/a><\/font> <\/p>\n<p align=\"justify\"><font size=\"5\">Heat is transferred by three mechanisms: conduction, convection, and radiation. <b>Conductio<\/b><b>n <\/b>is the transfer of energy from the more energetic particles of a substance to the adjacent less energetic ones as a result of interaction be- tween particles. <b>Convectio<\/b><b>n <\/b>is the transfer of energy between a solid surface and the adjacent fluid that is in motion, and it involves the combined effects of conduction and fluid motion. <b>Radiatio<\/b><b>n <\/b>is the transfer of energy due to the emission of electromagnetic waves (or photons).<\/font><\/p>\n","protected":false},"excerpt":{"rendered":"<p>Energy can be transferred to or from a closed system (a fixed mass) in two distinct forms: heat and work. For control volumes, energy can also be transferred by mass. An energy transfer to or from a closed system is heat if it is caused by a temperature difference between the system and its surroundings. 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