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| {{for|theoretical background|Heat pump and refrigeration cycle}}
| | == シャオヤンペースは、その体内で甘く魅力的です == |
| {{refimprove|date=August 2012}}
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| [[File:Heat Pump.jpg|thumb|265px|Outdoor components of a residential air-source heat pump]]
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| A '''heat pump''' is a device that provides heat energy from a source of heat to a destination called a "heat sink". Heat pumps are designed to move [[thermal energy]] opposite to the direction of spontaneous heat flow by absorbing heat from a cold space and release it to a warmer one, and vice-versa. A heat pump uses some amount of external power to accomplish the work of transferring energy from the heat source to the heat sink.
| | 泉は言った：「マルチ古い謝玄」。<br><br>「ああ、ほんの少しのことを、「玄香港の息子は微笑み、そして群衆に直面すると、手を振った。<br><br>見て、シャオは遠くない多くの人が滞在する行く、式典の後に行を曲げ、ゆっくりと会場を出さ<br><br>群衆を見て終了し、Xuankong息子はちょうど、微笑んささやいた： [http://www.ispsc.edu.ph/nav/japandi/casio-rakuten-2.html カシオ腕時計 g-shock] ''医学 [http://www.ispsc.edu.ph/nav/japandi/casio-rakuten-9.html 電波時計 casio] 'ほこり、私たちは、そのフィールドを賭けていた、彼らはダンがああチャンピオンになるこのセッションを取得することができシャオヤンと英二を見ている、私はあなたが私を獲得することができ、これを知らないのか？ [http://www.ispsc.edu.ph/nav/japandi/casio-rakuten-7.html カシオ 腕時計 gps] '<br><br>1132番目章魂のフィンガープリント<br><br>1132番目章魂のフィンガープリント<br>ホールの外<br>ライン、ストレートDantaをリード、あまりにも多くの話を持っていなかったシャオヤンと曹操Yingさんは、チャネルの底に行に直面している [http://www.ispsc.edu.ph/nav/japandi/casio-rakuten-13.html 時計 カシオ]。<br><br>'のように肖氏ヤン、と [http://www.ispsc.edu.ph/nav/japandi/casio-rakuten-8.html カシオ レディース 電波ソーラー腕時計]。'<br>ちょうど撮影し<br>シャオヤンペースは、その体内で甘く魅力的です |
| | 相关的主题文章： |
| | <ul> |
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| | <li>[http://www.zlslkj.com/plus/feedback.php?aid=65 http://www.zlslkj.com/plus/feedback.php?aid=65]</li> |
| | |
| | <li>[http://www.regalglass.com.cn/plus/feedback.php?aid=82 http://www.regalglass.com.cn/plus/feedback.php?aid=82]</li> |
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| | <li>[http://hablaameno.com/index.php/ http://hablaameno.com/index.php/]</li> |
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| | </ul> |
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| While [[air conditioner]]s and [[freezer]]s are familiar examples of heat pumps, the term "heat pump" is more general and applies to
| | == 薬「少し風が受信されない理由を分裂 == |
| many
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| [[HVAC]] devices used for space heating or space cooling. When a heat pump is used for heating, it employs the same basic [[Heat pump and refrigeration cycle|refrigeration-type cycle]] used by an air conditioner or a refrigerator, but in the opposite direction - releasing heat into the air-conditioned space rather than the surrounding environment. In this use, heat pumps generally draw heat from the cooler external air or from the ground.<ref>Air-source heat pumps|url=http://www.nrel.gov/docs/fy01osti/28037.pdf</ref>
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| ==Overview==
| | 無謀に長い間、単にハード飲み込んだ、7つの製品精錬 [http://www.ispsc.edu.ph/nav/japandi/casio-rakuten-9.html 電波時計 casio] '医学'分割後、修理を横になっていた遠くの行為を見て？限り、彼はすぐに開封したように、用超強力な幸せがたくさんあるでしょう、それは何も難しい問題であり、家に帰る道を破壊するために、人々のこの存在、彼らは震え助けておらず、ここで考えたショット、7つの製品精錬アピールの「医学」部門、誰も質問する勇気ない<br><br>薬「少し風が受信されない理由を分裂？？ [http://www.ispsc.edu.ph/nav/japandi/casio-rakuten-13.html カシオ腕時計 メンズ] 'チェン耀輝揮発顔」の他の精製このレベルに会ったが、この柳の家族」、飛行、7つの製品精錬「医学」部門のアイデアの心を左折、このファミリは、彼らの大きな男を呼び出すことができない、彼は理解することはできませんどのように、なぜ劉ファミリー、招待することができますか？<br>そう遠くない反対八尾ら中<br>、劉清、劉飛、歩行者は、あまりにも、彼がサポートされていない小燕の偶数ラウンドの手に実際にあるために、わずかに開いた口が地面上の距離を見て修理しなければならなかった |
| {{main|Heat pump and refrigeration cycle}}
| | 相关的主题文章： |
| In heating, ventilation and air conditioning ([[HVAC]]) applications, the term ''heat pump'' usually refers to easily reversible [[vapor-compression refrigeration]] devices optimized for high efficiency in both directions of thermal energy transfer.
| | <ul> |
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| | <li>[http://aiyingfang.cn/bbs/showtopic-883990.aspx http://aiyingfang.cn/bbs/showtopic-883990.aspx]</li> |
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| | <li>[http://www.law110.net/plus/feedback.php?aid=14 http://www.law110.net/plus/feedback.php?aid=14]</li> |
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| | <li>[http://lotus.raindrop.jp/cgi/joyful_exif/joyful.cgi http://lotus.raindrop.jp/cgi/joyful_exif/joyful.cgi]</li> |
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| | </ul> |
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| [[Heat]] spontaneously flows from warmer places to colder spaces. A heat pump can absorb heat from a cold space and release it to a warmer one, and vice-versa. "Heat" is not conserved in this process, which requires some amount of external high grade (low-entropy) energy, such as electricity.
| | == 心は「ボーッです == |
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| Heat pumps are used to provide heating because less high-grade energy is required for their operation than appears in the released heat. Most of the energy for heating comes from the external environment, and only a fraction comes from electricity (or some other high-grade energy source required to run a compressor). In electrically powered heat pumps, the heat transferred can be three or four times larger than the electrical power consumed, giving the system a Coefficient of Performance (COP) of 3 or 4, as opposed to a COP of 1 of a conventional electrical resistance heater, in which all heat is produced from input electrical energy.
| | 心は「ボーッです [http://www.ispsc.edu.ph/nav/japandi/casio-rakuten-8.html 時計 メンズ カシオ]<br><br>胡古い民謡を見たり、彫像の顔」の色」もすぐに冷笑沈ん9日は、この外観を見ていることを、明らかに、第一の以前の名前を聞いた [http://www.ispsc.edu.ph/nav/japandi/casio-rakuten-4.html カシオ ソーラー電波腕時計]。<br>9日間<br>「ねえ、家のあなたの魂を恐れて誰かが、私たちは、その日、地球恐れていない、あなたが本当に家の魂は唯一の完全に断片化できると思うか？ [http://www.ispsc.edu.ph/nav/japandi/casio-rakuten-14.html casio 腕時計 phys] '胡ボスPieliaopiezui、その後これと他の脅威を尊重しますが、追加された気にしなかった。<br><br>「Shaoge朱、ティムノイズがこの古い男は、私たちの3、そしてどのように、あなたの残りの3つを与えるのだろうか？ [http://www.ispsc.edu.ph/nav/japandi/casio-rakuten-11.html casio 腕時計 メンズ] '<br><br>胡、シャオヤンは微笑ん上司の言葉を聞いて、すぐにうなずいた、胡古い民謡が強いの3つの異なるレベルに対処するための星像の強さにあり、何か問題があってはなりません [http://www.ispsc.edu.ph/nav/japandi/casio-rakuten-14.html カシオ 時計 電波 ソーラー]。<br><br>「ハハ、その場合には、それが私たちの相手を解決する必要があります誰が見てだろう、「胡ボス笑い、体執念深圧倒的な高潮のうち、すぐにまっすぐに |
| | | 相关的主题文章： |
| Heat pumps use a refrigerant as an intermediate fluid to absorb heat where it vaporizes, in the evaporator, and then to release heat where the refrigerant condenses, in the condenser. The refrigerant flows through insulated pipes between the evaporator and the condenser, allowing for efficient thermal energy transfer at relatively long distances.
| | <ul> |
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| ===Reversible heat pumps===
| | <li>[http://www.halaosi.com/forum.php?mod=viewthread&tid=89188 http://www.halaosi.com/forum.php?mod=viewthread&tid=89188]</li> |
| Reversible heat pumps work in either thermal direction to provide heating or cooling to the internal space. They employ a [[reversing valve]] to reverse the flow of refrigerant from the compressor through the condenser and evaporation coils.
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| | | <li>[http://www.yunheshuyuan.com/bbs/home.php?mod=space&uid=1334314 http://www.yunheshuyuan.com/bbs/home.php?mod=space&uid=1334314]</li> |
| * In '''heating mode,''' the outdoor coil is an evaporator, while the indoor is a condenser. The refrigerant flowing from the evaporator (outdoor coil) carries the thermal energy from outside air (or soil) indoors, after the fluid's temperature has been augmented by compressing it. The indoor coil then transfers thermal energy (including energy from the compression) to the indoor air, which is then moved around the inside of the building by an [[air handler]]. Alternatively, thermal energy is transferred to water, which is then used to heat the building via radiators or [[underfloor heating]]. The heated water may also be used for [[domestic hot water]] consumption. The refrigerant is then allowed to expand, cool, and absorb heat to reheat to the outdoor temperature in the outside evaporator, and the cycle repeats. This is a standard refrigeration cycle, save that the "cold" side of the refrigerator (the evaporator coil) is positioned so it is outdoors where the environment is colder.
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| | | <li>[http://sunsb138.com/home.php?mod=space&uid=156849 http://sunsb138.com/home.php?mod=space&uid=156849]</li> |
| * In '''cooling mode''' the cycle is similar, but the outdoor coil is now the condenser and the indoor coil (which reaches a lower temperature) is the evaporator. This is the familiar mode in which air conditioners operate.
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| | | </ul> |
| ==Operating principles==
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| Mechanical heat pumps exploit the physical properties of a volatile evaporating and [[Condensation|condensing]] fluid known as a [[refrigerant]]. The heat pump compresses the refrigerant to make it hotter on the side to be warmed, and releases the pressure at the side where heat is absorbed. [[Image:Heatpump2.svg|thumb|300px|A simple stylized diagram of a heat pump's [[vapor-compression refrigeration]] cycle: 1) condenser, 2) expansion valve, 3) evaporator, 4) compressor.]] The working fluid, in its gaseous state, is pressurized and circulated through the system by a [[Gas compressor|compressor]]. On the discharge side of the compressor, the now hot and highly pressurized vapor is cooled in a [[heat exchanger]], called a [[Condenser (heat transfer)|condenser]], until it condenses into a high pressure, moderate temperature liquid. The condensed refrigerant then passes through a pressure-lowering device also called a metering device. This may be an [[Thermal expansion valve|expansion valve]], [[capillary]] tube, or possibly a work-extracting device such as a [[turbine]]. The low pressure liquid refrigerant then enters another heat exchanger, the evaporator, in which the fluid absorbs heat and boils. The refrigerant then returns to the compressor and the cycle is repeated.{{Citation needed|date=March 2011}}
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| It is essential that the refrigerant reaches a sufficiently high temperature, when compressed, to release heat through the "hot" heat exchanger (the condenser). Similarly, the fluid must reach a sufficiently low temperature when allowed to expand, or else heat cannot flow from the ambient cold region into the fluid in the cold heat exchanger (the evaporator). In particular, the pressure difference must be great enough for the fluid to condense at the hot side and still evaporate in the lower pressure region at the cold side. The greater the temperature difference, the greater the required pressure difference, and consequently the more energy needed to compress the fluid. Thus, as with all heat pumps, the [[Coefficient of Performance]] (amount of thermal energy moved per unit of input work required) decreases with increasing temperature difference.
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| [[Thermal insulation|Insulation]] is used to reduce the work and energy required to achieve a low enough temperature in the space to be cooled.
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| To operate in different temperature conditions, different refrigerants are available. Refrigerators, air conditioners, and some heating systems are common applications that use this technology.{{Citation needed|date=March 2011}}
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| ===Heat transport===
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| Heat is typically transported through engineered heating or cooling systems by using a flowing gas or liquid. Air is sometimes used, but quickly becomes impractical under many circumstances because it requires large ducts to transfer relatively small amounts of heat. In systems using refrigerant, this working fluid can also be used to transport heat a considerable distance, though this can become impractical because of increased risk of expensive refrigerant leakage. When large amounts of heat are to be transported, water is typically used, often supplemented with [[antifreeze]], [[corrosion inhibitors]], and other additives.
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| ===Heat sources/sinks===
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| A common source or sink for heat in smaller installations is the outside air, as used by an air-source heat pump. A fan is needed to improve heat exchange efficiency.
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| Larger installations handling more heat, or in tight physical spaces, often use water-source heat pumps. The heat is sourced or rejected in water flow, which can carry much larger amounts of heat through a given pipe or duct cross-section than air flow can carry. The water may be heated at a remote location by [[boiler]]s, [[solar energy]], or other means. Alternatively when needed, the water may be cooled by using a [[cooling tower]], or discharged into a large body of water, such as a lake or stream.
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| [[Geothermal heat pump]]s or ground-source heat pumps use shallow underground heat exchangers as a heat source or sink, and water as the heat transport medium. This is possible because below ground level, the temperature is relatively constant across the seasons, and the earth can provide or absorb a large amount of heat. Ground source heat pumps work in the same way as air-source heat pumps, but exchange heat with the ground via water pumped through pipes in the ground. Ground source heat pumps are simpler and more reliable than air source heat pumps - they do not need fan systems or defrosting systems and can be housed inside - but the need for a ground heat exchanger requires a higher initial capital cost in exchange for lower annual running costs as well-designed ground source heat pump systems enjoy a more efficient operation.
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| Heat pump installations may be installed alongside an auxiliary conventional heat source such as electrical resistance heaters, or oil or gas combustion. The auxiliary source is installed to meet peak heating loads, or to provide a back-up system.
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| ==Applications==
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| ===HVAC===
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| In [[HVAC]] applications, a heat pump is typically a [[vapor-compression refrigeration]] device that includes a reversing valve and optimized heat exchangers so that the direction of ''heat flow'' (thermal energy movement) may be reversed. The reversing valve switches the direction of refrigerant through the cycle and therefore the heat pump may deliver either heating or cooling to a building. In cooler climates, the default setting of the reversing valve is heating. The default setting in warmer climates is cooling. Because the two heat exchangers, the condenser and evaporator, must swap functions, they are optimized to perform adequately in both modes. Therefore, the [[SEER|efficiency]] of a reversible heat pump is typically slightly less than two separately optimized machines.
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| ===Plumbing===
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| In [[plumbing]] applications, a heat pump is sometimes used to heat or preheat water for swimming pools or [[Water heating|domestic water heater]]s; the heat energy removed from an air-conditioned space may be recovered for water heating.
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| ==Refrigerants==
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| Until the 1990s, the [[refrigerant]]s were often [[chlorofluorocarbon]]s such as R-12 ([[dichlorodifluoromethane]]), one in a class of several refrigerants using the brand name [[Freon]], a trademark of [[DuPont]]. Its manufacture was discontinued in 1995 because of the [[ozone depletion|damage]] that [[CFCs]] cause to the [[ozone layer]] if released into the [[Earth's atmosphere|atmosphere]].
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| One widely adopted replacement refrigerant is the hydrofluorocarbon (HFC) known as [[R-134a]] (1,1,1,2-tetrafluoroethane). Heat pumps using R-134a are not as efficient as those using R-12 that they replace (in automotive applications) and therefore, more energy is required to operate systems utilizing R-134a than those using R-12. Other substances such as liquid R-717 [[ammonia]] are widely used in large-scale systems, or occasionally the less corrosive but more flammable [[propane]] or [[butane]], can also be used.
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| Since 2001, [[carbon dioxide]], [[R-744]], has increasingly been used, utilizing the [[transcritical cycle]], although it requires much higher working pressures. In residential and commercial applications, the hydrochlorofluorocarbon (HCFC) R-22 is still widely used, however, HFC [[R-410A]] does not deplete the ozone layer and is being used more frequently. Hydrogen, helium, nitrogen, or plain air is used in the [[Stirling engine#Stirling cryocoolers|Stirling cycle]], providing the maximum number of options in environmentally friendly gases.
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| More recent refrigerators use [[R600A]] which is [[isobutane]], and does not deplete the ozone and is friendly to the environment.{{Citation needed|date=March 2011}}
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| [[Dimethyl ether]] (DME) is also gaining popularity as a refrigerant.<ref name="mecanica-dme">http://www.mecanica.pub.ro/frigo-eco/R404A_DME.pdf 101110</ref>
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| ==Efficiency==
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| When comparing the performance of heat pumps, it is best to avoid the word "efficiency", which has a very specific thermodynamic definition. The term [[coefficient of performance]] (COP) is used to describe the ratio of useful heat movement per work input. Most vapor-compression heat pumps use electrically powered motors for their work input. However, in many vehicle applications, mechanical energy from an [[internal combustion engine]] provides the needed work.
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| When used for heating a building on a mild day, for example 10 °C, a typical [[air-source heat pump]] (ASHP) has a COP of 3 to 4, whereas an electrical resistance [[heater]] has a COP of 1.0. That is, one [[joule]] of electrical energy will cause a resistance heater to produce only one joule of useful heat, while under ideal conditions, one joule of electrical energy can cause a heat pump to move much more than one joule of heat from a cooler place to a warmer place. Note that an air source heat pump is more efficient in hotter climates than cooler ones, so when the weather is much warmer the unit will perform with a higher COP (as it has less work to do). Conversely in extreme cold weather the COP approaches 1. Thus when there is a wide temperature differential between the hot and cold reservoirs, the COP is lower (worse).
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| On the other hand, [[ground-source heat pump]]s (GSHP) benefit from the moderated temperature underground, as the ground acts naturally as a store of thermal energy.<ref>Thermalbanks and Thermal Energy Storage, http://www.icax.co.uk/ThermalBanks.html</ref> Their year-round COP is therefore normally in the range of 2.5 to 5.0.
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| When there is a high temperature differential on a cold day, (e.g., when an air-source heat pump is used to heat a house on a cold winter day of 0 °C (32 °F)), it takes more work to move the same amount of heat to indoors than on a mild day. Ultimately, due to [[Carnot cycle|Carnot efficiency]] limits, the heat pump's performance will approach 1.0 as the outdoor-to-indoor temperature difference increases for colder climates (outside temperature gets colder). This typically occurs around −18 °C (0 °F) outdoor temperature for air source heat pumps.
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| Also, as the heat pump takes heat out of the air, some moisture in the outdoor air may condense and possibly freeze on the outdoor heat exchanger. The system must periodically melt this ice. When it is extremely cold outside, it is simpler, and wears the machine less, to heat using an electric-resistance heater rather than to overload an air-source heat pump.
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| The design of the evaporator and condenser heat exchangers is also very important to the overall efficiency of the heat pump. The heat exchange surface areas and the corresponding temperature differential (between the refrigerant and the air stream) directly affect the operating pressures and hence the work the compressor has to do in order to provide the same heating or cooling effect. Generally, the larger the heat exchanger the lower the temperature differential and the more efficient the system becomes.
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| Heat exchangers are expensive, requiring drilling for some heat-pump types or large spaces to be efficient, and the heat pump industry generally competes on price rather than efficiency. Heat pumps are already at a price disadvantage when it comes to initial investment (not long-term savings) compared to conventional heating solutions like boilers, so the drive towards more efficient heat pumps and air conditioners is often led by legislative measures on minimum efficiency standards.<ref>[[BSRIA]], "European energy legislation explained", www.bsria.co.uk, May 2010.</ref>
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| In cooling mode, a heat pump's operating performance is described in the US as its [[energy efficiency ratio]] (EER) or [[seasonal energy efficiency ratio]] (SEER), and both measures have units of BTU/(h·W) (1 BTU/(h·W) = 0.293 W/W). A larger EER number indicates better performance. The manufacturer's literature should provide both a COP to describe performance in heating mode, and an EER or SEER to describe performance in cooling mode. Actual performance varies, however, and depends on many factors such as installation, temperature differences, site elevation, and maintenance.
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| Heat pumps are more ''effective'' for heating than for cooling an interior space if the temperature differential is held equal. This is because the compressor's input energy is also converted to useful heat when in heating mode, and is discharged along with the transported heat via the condenser to the interior space. But for cooling, the condenser is normally outdoors, and the compressor's dissipated work (waste heat) must also be transported to outdoors using more input energy, rather than being put to a useful purpose. For the same reason, opening a food refrigerator or freezer actually heats up the room rather than cooling it because its refrigeration cycle rejects heat to the indoor air. This heat includes the compressor's dissipated work as well as the heat removed from the inside of the appliance.
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| The COP for a heat pump in a heating or cooling application, with steady-state operation, is:
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| :<math>
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| COP_\text{heating} = \frac{\Delta Q_\text{hot}}{\Delta A} \leq \frac{T_\text{hot}}{T_\text{hot}-T_\text{cool}},
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| </math>
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| :<math>
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| COP_\text{cooling} = \frac{\Delta Q_\text{cool}}{\Delta A} \leq \frac{T_\text{cool}}{T_\text{hot}-T_\text{cool}},
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| </math>
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| where
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| * <math>\Delta Q_\text{cool}</math> is the amount of heat extracted from a cold reservoir at temperature <math>T_\text{cool}</math>,
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| * <math>\Delta Q_\text{hot}</math> is the amount of heat delivered to a hot reservoir at temperature <math>T_\text{hot}</math>,
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| * <math>\Delta A</math> is the compressor's dissipated work.
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| * All temperatures are absolute temperatures usually measured in [[kelvin]]s or degrees [[Rankine scale|Rankine]].
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| ===Coefficient of performance (COP) and lift===
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| The COP increases as the temperature difference, or "lift", decreases between heat source and destination. The COP can be maximized at design time by choosing a heating system requiring only a low final water temperature (e.g. underfloor heating), and by choosing a heat source with a high average temperature (e.g. the ground). Domestic hot water (DHW) and conventional heating radiators require high water temperatures, reducing the COP that can be attained, and affecting the choice of heat pump technology.{{Citation needed|date=March 2011}}
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| {| class="wikitable" style="text-align:center; margin-right:auto"
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| |+ COP variation with output temperature
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| |-
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| ! scope="col" | Pump type and source
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| ! scope="col" | Typical use
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| ! scope="col" | 35 °C <br> (e.g. heated screed floor)
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| ! scope="col" | 45 °C <br> (e.g. heated screed floor)
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| ! scope="col" | 55 °C <br> (e.g. heated timber floor)
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| ! scope="col" | 65 °C <br> (e.g. radiator or [[Water heating|DHW]])
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| ! scope="col" | 75 °C <br> (e.g. radiator and DHW)
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| ! scope="col" | 85 °C <br> (e.g. radiator and DHW)
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| |-
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| |style="text-align:left"| High-efficiency air source heat pump (ASHP), air at −20 °C<ref name="CREN">The Canadian Renewable Energy Network [http://dsp-psd.pwgsc.gc.ca/Collection/M92-251-2002E.pdf 'Commercial Earth Energy Systems', Figure 29]. . Retrieved December 8, 2009.</ref>
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| |style="text-align:left"|
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| | 2.2
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| |style="text-align:left"| Two-stage ASHP, air at −20 °C<ref name="TIPC">Technical Institute of Physics and Chemistry, Chinese Academy of Sciences [http://repository.tamu.edu/bitstream/handle/1969.1/5474/ESL-IC-06-11-312.pdf?sequence=4 'State of the Art of Air-source Heat Pump for Cold Region', Figure 5]. . Retrieved April 19, 2008.</ref>
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| |style="text-align:left"| Low source temperature
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| | ''2.4''
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| | 1.9
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| |style="text-align:left"| High efficiency ASHP, air at 0 °C<ref name="CREN"/>
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| |style="text-align:left"| Low output temperature
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| | ''3.8''
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| |-
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| |style="text-align:left"| Prototype transcritical {{chem|CO|2}} (R744) heat pump with tripartite gas cooler, source at 0 °C<ref name="STEEN">SINTEF Energy Research [http://www.r744.com/knowledge/papers/files/pdf/pdf_379.pdf 'Integrated CO<sub>2</sub> Heat Pump Systems for Space Heating and DHW in low-energy and passive houses', J. Steen, Table 3.1, Table 3.3]. . Retrieved April 19, 2008.</ref>
| |
| |style="text-align:left"| High output temperature
| |
| | 3.3
| |
| | ‐
| |
| | ‐
| |
| | ''4.2''
| |
| | ‐
| |
| | 3.0
| |
| |-
| |
| |style="text-align:left"| Ground source heat pump (GSHP), water at 0 °C<ref name="CREN"/>
| |
| |style="text-align:left"|
| |
| | 5.0
| |
| | 3.7
| |
| | 2.9
| |
| | 2.4
| |
| | ‐
| |
| | ‐
| |
| |-
| |
| |style="text-align:left"| GSHP, ground at 10 °C<ref name="CREN"/>
| |
| |style="text-align:left"| Low output temperature
| |
| | ''7.2''
| |
| | 5.0
| |
| | 3.7
| |
| | 2.9
| |
| | 2.4
| |
| | ‐
| |
| |-
| |
| |style="text-align:left"| Theoretical [[Carnot cycle]] limit, source −20 °C
| |
| |style="text-align:left"|
| |
| | 5.6
| |
| | 4.9
| |
| | 4.4
| |
| | 4.0
| |
| | 3.7
| |
| | 3.4
| |
| |-
| |
| |style="text-align:left"| Theoretical [[Carnot cycle]] limit, source 0 °C
| |
| |style="text-align:left"|
| |
| | 8.8
| |
| | 7.1
| |
| | 6.0
| |
| | 5.2
| |
| | 4.6
| |
| | 4.2
| |
| |-
| |
| |style="text-align:left"| Theoretical [[Transcritical cycle|Lorentzen cycle]] limit ({{chem|CO|2}} pump), return fluid 25 °C, source 0 °C<ref name="STEEN"/>
| |
| |style="text-align:left"|
| |
| | 10.1
| |
| | 8.8
| |
| | 7.9
| |
| | 7.1
| |
| | 6.5
| |
| | 6.1
| |
| |-
| |
| |style="text-align:left"| Theoretical [[Carnot cycle]] limit, source 10 °C
| |
| |style="text-align:left"|
| |
| | 12.3
| |
| | 9.1
| |
| | 7.3
| |
| | 6.1
| |
| | 5.4
| |
| | 4.8
| |
| |}
| |
| | |
| One observation is that while current "best practice" heat pumps (ground source system, operating between 0 °C and 35 °C) have a typical COP around 4, no better than 5, the maximum achievable is 8.8 because of fundamental [[Carnot cycle]] limits. This means that in the coming decades, the energy efficiency of top-end heat pumps could at least double. Cranking up efficiency requires the development of a better [[gas compressor]], fitting HVAC machines with larger heat exchangers with slower gas flows, and solving internal [[lubrication]] problems resulting from slower gas flow.
| |
| Depending on the working fluid, the expansion stage can be important also. Work done by the expanding fluid cools it and is available to replace some of the input power. (An evaporating liquid is cooled by free expansion through a small hole, but an ideal gas is not.)
| |
| | |
| ==Types==
| |
| | |
| ===Compression v. absorption===
| |
| The two main types of heat pumps are [[Gas compression|compression]] and absorption. Compression heat pumps operate on mechanical energy (typically driven by electricity), while absorption heat pumps may also run on heat as an energy source (from electricity or burnable fuels).<ref>http://www2.vlaanderen.be/economie/energiesparen/doc/brochure_warmtepomp.pdf</ref> An absorption heat pump may be fueled by [[natural gas]] or [[LP gas]], for example. While the Gas Utilization Efficiency in such a device, which is the ratio of the energy supplied to the energy consumed, may average only 1.5; that is better than a natural gas or LP gas furnace, which can only approach 1.
| |
| | |
| Although an [[absorption refrigerator|absorption]] heat pump may not be as efficient as an electric compression heat pump, an absorption heat pump fueled by natural gas may be advantageous in locations where electricity is relatively expensive and natural gas is relatively inexpensive. A natural gas-fired absorption heat pump might also avoid the cost of an electrical service upgrade which is sometimes necessary for an electric heat pump installation. In the case of air-to-air heat pumps, an absorption heat pump might also have an advantage in colder regions, due to a lower minimum [[operating temperature]].<ref>[http://www.robur.com/technology/heat-pumps-comparison/page-3.html ROBUR heat pumps comparison]</ref>
| |
| | |
| ==Heat sources and sinks==
| |
| By definition, all heat sources for a heat pump must be colder in temperature than the space to be heated. Most commonly, heat pumps draw heat from the air (outside or inside air) or from the ground ([[groundwater]] or [[soil]]).<ref>{{cite web|url=http://www2.vlaanderen.be/economie/energiesparen/doc/folder_warmtepomp.pdf |title=Heat pumps sources including groundwater, soil, outside and inside air) |format=PDF |date= |accessdate=2010-06-02}}</ref>
| |
| | |
| The heat drawn from ground-sourced systems is in most cases stored solar heat, and it should not be confused with direct [[geothermal]] heating, though the latter will contribute in some small measure to all heat in the ground. True geothermal heat, when used for heating, requires a circulation pump but no heat pump, since for this technology the ground temperature is higher than that of the space that is to be heated, so the technology relies only upon simple [[heat convection]].
| |
| | |
| Other heat sources for heat pumps include water; nearby streams and other natural water bodies have been used, and sometimes domestic waste water (via [[drain water heat recovery]]) which is often warmer than cold winter ambient temperatures (though still of lower temperature than the space to be heated).
| |
| | |
| A number of sources have been used for the heat source for heating private and communal buildings.<ref>[http://www1.eere.energy.gov/geothermal/pdfs/26161b.pdf Homeowners using heat pump systems]{{Dead link|date=June 2010}}</ref>
| |
| | |
| ===Air (ASHP)===
| |
| {{Main|Air source heat pumps}}
| |
| | |
| * Air source heat pump (extracts heat from outside air)
| |
| ** Air–air heat pump (transfers heat to inside air)
| |
| ** Air–water heat pump (transfers heat to a heating circuit and a tank of domestic hot water)
| |
| | |
| There are thus two types of air source heat pumps and these are commonly clearly separate types of devices. Both devices use outside air as the heat source. Air-air heat pumps, that extract heat from outside air and transfer this heat to inside air, are the most common type of heat pumps and the cheapest. These do not have other major differences from [[air conditioner]]s than that their purpose is to heat the inside air instead of cooling it: they transfer heat into a building as compared to air conditioners which transfer heat out of a building. Air-air heat pumps often have the capability of cooling as it is just the same process, but just in the opposite direction. Air-water heat pumps are otherwise similar to air-air heat pumps, but they transfer the extracted heat into a heating circuit, [[floor heating]] being the most efficient, and they can also transfer heat into a domestic hot water tank and this water is consequently used in the shower and hot water taps of the building. However, ground-water heat pumps are more efficient than air-water heat pumps, and therefore the former is most often the better choice for providing heat for the floor heating and domestic hot water systems.
| |
| | |
| Air source heat pumps are relatively easy and inexpensive to install and have therefore historically been the most widely used heat pump type. However, they suffer limitations due to their use of the outside air as a heat source. The higher temperature differential during periods of extreme cold or heat leads to declining efficiency, as explained above. In mild weather, [[Coefficient of performance|COP]] may be around 4.0, while at temperatures below around 0 °C (32 °F) an air-source heat pump can achieve a COP of 2.5 or better, which is considerably more than the energy efficiency that may be achieved by a 1980's heating systems, and very similar to state of the art oil or gas heaters.<ref>EnergyIdeas.org, "[http://www.energyideas.org/documents/Factsheets/PTR/AcadiaHeatPump.pdf Product & Technology Review: Acadia Heat Pump]", Table 1, Dec 2007.</ref> The average COP over seasonal variation is typically 2.5-2.8, with exceptional models able to exceed 6.0 in very mild climate, but not in freezing climates.<ref>{{cite web|url=http://www.ipcc.ch/pdf/assessment-report/ar4/wg3/ar4-wg3-chapter6.pdf |title=the IPCC 4th Working Group III report |format=PDF |date= |accessdate=2010-06-02}}</ref>
| |
| | |
| At least two manufacturers are selling heat pumps that maintain better heating output at lower outside temperatures than conventional air source heat pumps. These low temperature optimized models make air source heat pumps more practical for cold climates because they do not freeze and shut down as readily. Some models however, defrost their outdoor unit using electrical resistance heating at regular intervals, which increases electricity consumption dramatically during the coldest periods. In areas where only one fossil fuel is currently available (e.g. heating oil only; no natural gas pipes available) these heat pumps could be used as an alternative, supplemental heat source to reduce a building's direct dependence on fossil fuel. Depending on fuel and electricity prices, using the heat pump for heating may be less expensive than fossil fuel. A backup fossil-fuel, solar hot water or biomass heat source may still be required for the coldest days.{{Citation needed|date=March 2011}}
| |
| | |
| The heating output of low temperature optimized heat pumps (and hence their energy efficiency) still declines dramatically as the temperature drops, but the threshold at which the decline starts is lower than conventional pumps, as shown in the following table (temperatures are approximate and may vary by manufacturer and model):
| |
| | |
| {| class="wikitable"
| |
| |-
| |
| ! Air Source Heat Pump Type !! Full heat output at or above this temperature !! Heat output down to 60% of maximum at
| |
| |-
| |
| | Conventional || 47 °F (8.3 °C) || 32 °F (0 °C)
| |
| |-
| |
| | Low Temp Optimized || 41 °F ( 5 °C) || 17 °F (-8.3 °C)
| |
| |}
| |
| | |
| ===Ground (GSHP)===
| |
| {{Main|Ground-source heat pump}}
| |
| | |
| * Ground source heat pump (extracts heat from the ground or similar sources)
| |
| ** Ground–air heat pump (transfers heat to inside air)
| |
| *** Soil–air heat pump (soil as a source of heat)
| |
| *** Rock–air heat pump (rock as a source of heat)
| |
| *** Water–air heat pump (body of water as a source of heat, can be [[groundwater]], [[lake]], [[river]] etc.)
| |
| ** Ground–water heat pump (transfers heat to a heating circuit and a tank of domestic hot water)
| |
| *** Soil–water heat pump (ground as a source of heat)
| |
| *** Rock–water heat pump (rock as a source of heat)
| |
| *** Water–water heat pump (body of water as a source of heat)
| |
| | |
| Ground-source heat pumps, also called geothermal heat pumps, typically have higher efficiencies than air-source heat pumps. This is because they draw heat from the ground or [[groundwater]] which is at a relatively constant temperature all year round below a depth of about 30 feet (9 m).<ref>Earth Temperature and Site Geology, http://www.geo4va.vt.edu/A1/A1.htm</ref> This means that the temperature differential is lower, leading to higher efficiency. Ground-source heat pumps typically have COPs of 3.0<ref>http://www.hydro.mb.ca/regulatory_affairs/electric/gra_2012_2013/Appendix_38.pdf</ref> at the beginning of the heating season, with lower COPs as heat is drawn from the ground. The tradeoff for this improved performance is that a ground-source heat pump is more expensive to install, due to the need for the drilling of boreholes for vertical placement of heat exchanger piping or the digging of trenches for horizontal placement of the piping that carries the heat exchange fluid (water with a little antifreeze).
| |
| | |
| When compared, groundwater heat pumps are generally more efficient than heat pumps using heat from the soil. Closed loop soil or ground heat exchangers tend to accumulate cold, which is a significant problem if nearby ground water is stagnant or the soil lacks thermal conductivity, and the overall system has been designed to be just big enough to handle a "typical worst case" cold spell, or is simply undersized for the load.<ref>http://geothermalhelp.com/sizing-a-geothermal-heating-system/</ref> One way to fix cold accumulation in the ground heat exchanger loop, is to use ground water to cool the floors of the building on hot days, thereby transferring heat from the dwelling into the ground loop. There are several other methods for replenishing a low temperature ground loop; one way is to make large solar collectors, for instance by putting plastic pipes just under the roof, or by putting coils of black polyethylene pipes under glass on the roof, or by piping the tarmac of the parking lot.<ref>http://www.icax.co.uk/asphalt_solar_collector.html</ref> The most cost-effective way is to put a large air-to-water heat exchanger on the rooftop.{{Citation needed|date=March 2011}}
| |
| | |
| ===Exhaust air (EAHP)===
| |
| {{Main|Exhaust air heat pump}}
| |
| | |
| * Exhaust air heat pump (extracts heat from the exhaust air of a building, requires [[Ventilation (architecture)|mechanical ventilation]])
| |
| ** Exhaust air-air heat pump (transfers heat to intake air)
| |
| ** Exhaust air-water heat pump (transfers heat to a heating circuit and a tank of domestic hot water)
| |
| | |
| ===Water source heat pumps (WSHP)===
| |
| | |
| * Uses flowing water as source or sink for heat
| |
| * Single-pass vs. recirculation
| |
| ** Single-pass — water source a body of water or a stream
| |
| ** Recirculation
| |
| *** When cooling, closed-loop heat transfer medium to central [[cooling tower]] or [[chiller]] (typically in a building or industrial setting)
| |
| *** When heating, closed-loop heat transfer medium from central boilers generating heat from combustion or other sources
| |
| | |
| ===Hybrid (HHP)===
| |
| | |
| Hybrid (or twin source) heat pumps: when outdoor air is above 4 to 8 Celsius, (40-50 Fahrenheit, depending on ground water temperature) they use air; when air is colder, they use the ground source. These twin source systems can also store summer heat, by running ground source water through the air exchanger or through the building heater-exchanger, even when the heat pump itself is not running. This has dual advantage: it functions as a low running cost for air cooling, and (if ground water is relatively stagnant) it cranks up the temperature of the ground source, which improves the energy efficiency of the heat pump system by roughly 4 percent for each degree in temperature rise of the ground source.
| |
| | |
| ===Air/water-brine/water heat pump (hybrid heat pump)===
| |
| | |
| The air/water-brine/water heat pump is a hybrid heat pump that uses only renewable energy sources in their execution. It combines air and geothermal heat in one compact device. Thus, this hybrid system differs from other systems that also use at least two heat sources. These usually form a mix of conventional heating (gas condensing technology) and renewable energy sources. The air/water-brine/water heat pump (hybrid heat pump) is equipped with two evaporators (an outside air evaporator and a brine evaporator), both of which are connected to the heat pump cycle.
| |
| This allows, in comparison with the external conditions (for example air temperature) to use the current time to the most economical heating source priority. The unit automatically selects the most efficient operating mode (air or geothermal heat). Depending on the mode of operation of the air and geothermal energy sources can be used simultaneously or alternatively. This process is controlled by a control unit. It processes large amounts of data that are incurred in the complex heating system, and consists of two controllers, one for the air heat cycle and one for the geothermal circulation. The two controllers are combined in one device and communicate permanently in the BUS-system, which ensures an efficiency-enhancing interaction of all components in the hybrid heating system.
| |
| The German Patent and Trade Mark Office in Munich granted a patent for the 2008 in Rostock (East Germany) developed air/water-brine/water heat pump (hybrid heat pump) under the title “Heat pump and method for controlling the source inlet temperature to the heat pump”. The air/water-brine/water heat pump (hybrid heat pump) can be combined with a solar thermal system or with an ice-storage.
| |
| The air/water-brine/water heat pump (hybrid heat pump) trades and marketed under the name ThermSelect. In United Kingdom was ThermSelect one of the winners of the 2013 HVR Awards for Excellence, organised by Heating and Ventilating Review – the essential reading for all those involved in the heating and ventilating industry. In sector for the Commercial Heating Product of the Year the award went to ThermSelect, the dual air and ground source heat pump within one unit.
| |
| | |
| ==Heat distribution==
| |
| {{unreferenced section|date=January 2011}}
| |
| Heat pumps are only highly efficient when they generate heat at a low temperature differential, ideally around or below {{convert|32|°C|°F}}. Normal steel plate radiators are not practical, because they would need to be four to six times their current size. Underfloor heating is one ideal solution. When wooden floors or carpets would spoil efficiency, wall heaters (plastic pipes covered with a thick layer of chalk) and piped ceilings can be used. These systems have the disadvantage that they are slow starters, and that they would require extensive renovation in existing buildings.
| |
| | |
| The alternative is a warm air system.
| |
| Such a setup can either complement slower floor heating during warm up, or it can be a quick and economical way to implement a heat pump system into existing buildings. Oversizing the fans and ductwork can reduce the [[acoustic noise]] they produce. To efficiently distribute warm water or air from a heat pump, water pipes or air shafts must have significantly larger diameters than in conventional, hotter-source systems, and underfloor heaters should have much more pipes per square meter.{{Citation needed|date=March 2011}}
| |
| | |
| ==Solid state heat pumps==
| |
| | |
| ===Magnetic===
| |
| {{Main|Magnetic refrigeration}}
| |
| In 1881, the German physicist [[Emil Warburg]] put a block of iron into a strong magnetic field and found that it increased very slightly in temperature. Some commercial ventures to implement this technology are underway, claiming to cut energy consumption by 40% compared to current domestic refrigerators<!-- The article referenced is unclear what the reference "standard fridge" is -->.<ref>Guardian Unlimited, December 2006 [http://environment.guardian.co.uk/energy/story/0,,1971818,00.html 'A cool new idea from British scientists: the magnetic fridge']</ref> The process works as follows: Powdered [[gadolinium]] is moved into a magnetic field, heating the material by 2 to 5 °C (4 to 9 °F). The heat is removed by a circulating fluid. The material is then moved out of the magnetic field, reducing its temperature below its starting temperature.{{Citation needed|date=March 2011}}
| |
| | |
| ===Thermoelectric===
| |
| {{Main|Thermoelectric cooling|Thermoelectric materials}}
| |
| Solid state heat pumps using the [[thermoelectric effect]] have improved over time to the point where they are useful for certain refrigeration tasks. Thermoelectric (Peltier) heat pumps are generally only around 10-15% as efficient as the ideal [[refrigerator]] ([[Carnot cycle]]), compared with 40–60% achieved by conventional compression cycle systems (reverse [[Rankine cycle|Rankine]] systems using compression/expansion);<ref>http://www.pnl.gov/main/publications/external/technical_reports/pnnl-19259.pdf - The Prospects of Alternatives to Vapor Compression Technology for Space Cooling and Food Refrigeration Applications</ref> however, this area of technology is currently the subject of active research in materials science.
| |
| | |
| ===Thermoacoustic===
| |
| {{Main|Thermoacoustic hot air engine}}
| |
| Near-solid-state heat pumps using [[thermoacoustics]] are commonly used in cryogenic laboratories.{{Citation needed|date=March 2011}}
| |
| | |
| ==Historical development==
| |
| {{Expand section|date=June 2008}}
| |
| | |
| Milestones:
| |
| * 1748: [[William Cullen]] demonstrates artificial refrigeration.
| |
| * 1834: [[Jacob Perkins]] builds a practical [[refrigerator]] with [[diethyl ether]].
| |
| * 1852: [[William Thomson, 1st Baron Kelvin|Lord Kelvin]] describes the theory underlying heat pump.
| |
| * 1855–1857: [[Peter von Rittinger]] develops and builds the first heat pump.<ref>{{Cite book |last=Banks |first=David L. |authorlink=David L. Banks |title=An Introduction to Thermogeology: Ground Source Heating and Cooling |publisher=Wiley-Blackwell |isbn=978-1-4051-7061-1 }}</ref>
| |
| * 1940: [[Robert C. Webber]] is credited as developing and building the first ground heat pump.<ref>"History of Geothermal Technology." Energicity. 2010. http://www.energicity.net/Geo-History.html</ref>
| |
| | |
| ==See also==
| |
| {{Portal|Energy}}
| |
| {{div col|colwidth=30em}}
| |
| * [[EcoCute]] domestic heat pump water heater
| |
| * [[Züblin AG]] [[Energietübbing]]<ref>[http://www.energyforlondon.org/energietubbing-for-crossrail/ Energietübbing]</ref>
| |
| * [[Flash evaporation]]
| |
| * [[Geothermal heat pump]]
| |
| * [[Heat exchanger]]
| |
| * [[Renewable heat]]
| |
| * [[Thermoelectric]] heat pumps that use the [[Peltier effect]]
| |
| * [[Vapor-compression refrigeration]]
| |
| * [[Vortex tube]]
| |
| * [[IEA-ECBCS Annex 48 : Heat Pumping and Reversible Air Conditioning]]
| |
| {{div col end}}
| |
| | |
| ==References==
| |
| {{Reflist|2}}
| |
| | |
| ==External links==
| |
| {{Commons category|Heat pumps}}
| |
| * [http://www1.eere.energy.gov/geothermal/heatpumps.html Practical information on setting up geothermal heat pump systems at home]
| |
| * [http://geoexchange.us/illustrations/graphics.htm Pictures on private/communal heat pump installations]
| |
| * [http://www.heatpumpcentre.org/ International Energy Agency Heat Pump Programme, Information site for heat pumping technology]
| |
| | |
| [[Category:Heat pumps]]
| |
| [[Category:Building engineering]]
| |
| [[Category:Residential heating]]
| |