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此词条暂由彩云小译翻译,未经人工整理和审校,带来阅读不便,请见谅。'''Dissipation''' is the result of an [[irreversible process]] that takes place in homogeneous [[Thermodynamics|thermodynamic]] systems. A dissipative process is a process in which energy (internal, bulk flow kinetic, or system potential) is transformed from some initial form to some final form; the capacity of the final form to do mechanical work is less than that of the initial form. For example, [[Heat Transfer|heat transfer]] is dissipative because it is a transfer of internal energy from a hotter body to a colder one. Following the [[second law of thermodynamics]], the [[entropy]] varies with temperature (reduces the capacity of the combination of the two bodies to do mechanical work), but never decreases in an isolated system.
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此词条暂由彩云小译翻译,翻译字数共665,未经人工整理和审校,带来阅读不便,请见谅。
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Dissipation is the result of an irreversible process that takes place in homogeneous thermodynamic systems. A dissipative process is a process in which energy (internal, bulk flow kinetic, or system potential) is transformed from some initial form to some final form; the capacity of the final form to do mechanical work is less than that of the initial form. For example, heat transfer is dissipative because it is a transfer of internal energy from a hotter body to a colder one. Following the second law of thermodynamics, the entropy varies with temperature (reduces the capacity of the combination of the two bodies to do mechanical work), but never decreases in an isolated system.
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In [[thermodynamics]], '''dissipation''' is the result of an [[irreversible process]] that takes place in homogeneous [[Thermodynamic system|thermodynamic systems]]. A dissipative process is a process in which [[energy]] ([[Internal energy|internal]], bulk flow [[Kinetic energy|kinetic]], or system [[Potential energy|potential]]) is [[Energy transformation|transformed]] from some initial form to some final form; the capacity of the final form to do [[mechanical work]] is less than that of the initial form. For example, [[Heat Transfer|heat transfer]] is dissipative because it is a transfer of internal energy from a hotter body to a colder one. Following the [[second law of thermodynamics]], the [[entropy]] varies with [[temperature]] (reduces the capacity of the combination of the two bodies to do mechanical work), but never decreases in an isolated system.
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耗散是在均匀热力学系统中发生的不可逆性的结果。耗散过程是能量(内部、体流动动力学或系统势能)从某种初始形式转化为某种最终形式的过程,最终形式做机械功的能力小于初始形式。例如,热传递是耗散的,因为它是内部能量从一个较热的物体向一个较冷的物体的转移。在热力学第二定律之后,熵随温度变化(降低了两个物体组合做机械功的能力) ,但是在一个孤立的系统中熵不会减少。
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In thermodynamics, dissipation is the result of an irreversible process that takes place in homogeneous thermodynamic systems. A dissipative process is a process in which energy (internal, bulk flow kinetic, or system potential) is transformed from some initial form to some final form; the capacity of the final form to do mechanical work is less than that of the initial form. For example, heat transfer is dissipative because it is a transfer of internal energy from a hotter body to a colder one. Following the second law of thermodynamics, the entropy varies with temperature (reduces the capacity of the combination of the two bodies to do mechanical work), but never decreases in an isolated system.
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在热力学中,耗散是在均匀热力学系统中发生的不可逆性的结果。耗散过程是能量(内部、体流动动力学或系统势)从某种初始形式转化为某种最终形式的过程,最终形式做机械功的能力小于初始形式。例如,热传递是耗散的,因为它是内部能量从一个较热的物体向一个较冷的物体的转移。在热力学第二定律之后,熵随温度变化(降低了两个物体组合做机械功的能力) ,但是在一个孤立的系统中熵不会减少。
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These processes produce entropy (see [[entropy production]]) at a certain rate. The entropy production rate times ambient temperature gives the dissipated [[Power (physics)|power]]. Important examples of irreversible processes are: [[heat flow]] through a [[thermal resistance]], [[fluid flow]] through a flow resistance, diffusion (mixing), [[Chemical reaction|chemical reactions]], and [[Electric current|electrical current]] flow through an [[Electrical resistance and conductance|electrical resistance]] ([[Joule heating]]).
These processes produce entropy (see [[entropy production]]) at a certain rate. The entropy production rate times ambient temperature gives the dissipated power. Important examples of irreversible processes are: heat flow through a thermal resistance, fluid flow through a flow resistance, diffusion (mixing), chemical reactions, and electrical current flow through an electrical resistance (Joule heating).
      
These processes produce entropy (see entropy production) at a certain rate. The entropy production rate times ambient temperature gives the dissipated power. Important examples of irreversible processes are: heat flow through a thermal resistance, fluid flow through a flow resistance, diffusion (mixing), chemical reactions, and electrical current flow through an electrical resistance (Joule heating).
 
These processes produce entropy (see entropy production) at a certain rate. The entropy production rate times ambient temperature gives the dissipated power. Important examples of irreversible processes are: heat flow through a thermal resistance, fluid flow through a flow resistance, diffusion (mixing), chemical reactions, and electrical current flow through an electrical resistance (Joule heating).
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{{Wiktionary}}
 
{{Wiktionary}}
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== Definition ==
      
== Definition ==
 
== Definition ==
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定义
      
Thermodynamic dissipative processes are essentially irreversible. They [[entropy production|produce entropy]] at a finite rate. In a process in which the temperature is locally continuously defined, the local density of rate of entropy production times local temperature gives the local density of dissipated power.[Definition needed!]
 
Thermodynamic dissipative processes are essentially irreversible. They [[entropy production|produce entropy]] at a finite rate. In a process in which the temperature is locally continuously defined, the local density of rate of entropy production times local temperature gives the local density of dissipated power.[Definition needed!]
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热力学耗散过程本质上是不可逆的。它们以有限的速率产生熵。在一个局部连续定义温度的过程中,产生熵的局部密度乘以局部温度得到局部耗散功率密度。[需要定义! ]
 
热力学耗散过程本质上是不可逆的。它们以有限的速率产生熵。在一个局部连续定义温度的过程中,产生熵的局部密度乘以局部温度得到局部耗散功率密度。[需要定义! ]
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耗散过程的特殊现象不能用单个的哈密顿形式来描述。耗散过程需要一系列可接受的个体哈密顿描述,准确地描述未知的兴趣过程的实际特殊发生。这包括摩擦力,以及所有导致能量退相干的类似作用力---- 也就是说,相干或定向能量流转化为间接或更为各向同性的能量分布。
 
耗散过程的特殊现象不能用单个的哈密顿形式来描述。耗散过程需要一系列可接受的个体哈密顿描述,准确地描述未知的兴趣过程的实际特殊发生。这包括摩擦力,以及所有导致能量退相干的类似作用力---- 也就是说,相干或定向能量流转化为间接或更为各向同性的能量分布。
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=== Energy ===
 
=== Energy ===
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=== Energy ===
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能源
      
"The conversion of mechanical energy into heat is called energy dissipation." – ''François Roddier''<ref>[http://www.editions-parole.net/?product=thermodynamique-de-levolution-un-essai-de-thermo-bio-sociologie Roddier F., ''Thermodynamique de l'évolution (The Thermodynamics of Evolution)'', parole éditions, 2012]</ref> The term is also applied to the loss of energy due to generation of unwanted heat in electric and electronic circuits.
 
"The conversion of mechanical energy into heat is called energy dissipation." – ''François Roddier''<ref>[http://www.editions-parole.net/?product=thermodynamique-de-levolution-un-essai-de-thermo-bio-sociologie Roddier F., ''Thermodynamique de l'évolution (The Thermodynamics of Evolution)'', parole éditions, 2012]</ref> The term is also applied to the loss of energy due to generation of unwanted heat in electric and electronic circuits.
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"The conversion of mechanical energy into heat is called energy dissipation." – François Roddier The term is also applied to the loss of energy due to generation of unwanted heat in electric and electronic circuits.
 
"The conversion of mechanical energy into heat is called energy dissipation." – François Roddier The term is also applied to the loss of energy due to generation of unwanted heat in electric and electronic circuits.
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机械能转化为热量的过程叫做能量耗散- 弗朗索瓦 · 罗迪埃这个术语也用于指电子电路中由于产生不必要的热量而造成的能量损失
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机械能转化为热量的过程叫做能量耗散这一术语也用于指电子电路中由于产生不需要的热量而造成的能量损失
 
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=== Computational physics ===
 
=== Computational physics ===
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=== Computational physics ===
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计算物理学
      
In [[computational physics]], numerical dissipation (also known as "numerical diffusion") refers to certain side-effects that may occur as a result of a numerical solution to a differential equation. When the pure [[advection]] equation, which is free of dissipation, is solved by a numerical approximation method, the energy of the initial wave may be reduced in a way analogous to a diffusional process. Such a method is said to contain 'dissipation'. In some cases, "artificial dissipation" is intentionally added to improve the [[numerical stability]] characteristics of the solution.<ref>Thomas, J.W. Numerical Partial Differential Equation: Finite Difference Methods. Springer-Verlag. New York. (1995)</ref>
 
In [[computational physics]], numerical dissipation (also known as "numerical diffusion") refers to certain side-effects that may occur as a result of a numerical solution to a differential equation. When the pure [[advection]] equation, which is free of dissipation, is solved by a numerical approximation method, the energy of the initial wave may be reduced in a way analogous to a diffusional process. Such a method is said to contain 'dissipation'. In some cases, "artificial dissipation" is intentionally added to improve the [[numerical stability]] characteristics of the solution.<ref>Thomas, J.W. Numerical Partial Differential Equation: Finite Difference Methods. Springer-Verlag. New York. (1995)</ref>
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In computational physics, numerical dissipation (also known as "numerical diffusion") refers to certain side-effects that may occur as a result of a numerical solution to a differential equation. When the pure advection equation, which is free of dissipation, is solved by a numerical approximation method, the energy of the initial wave may be reduced in a way analogous to a diffusional process. Such a method is said to contain 'dissipation'. In some cases, "artificial dissipation" is intentionally added to improve the numerical stability characteristics of the solution.
 
In computational physics, numerical dissipation (also known as "numerical diffusion") refers to certain side-effects that may occur as a result of a numerical solution to a differential equation. When the pure advection equation, which is free of dissipation, is solved by a numerical approximation method, the energy of the initial wave may be reduced in a way analogous to a diffusional process. Such a method is said to contain 'dissipation'. In some cases, "artificial dissipation" is intentionally added to improve the numerical stability characteristics of the solution.
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在计算物理学,数值耗散(也称为“数值扩散”)是指某些副作用,可能发生的结果,数值解的微分方程。用数值近似方法求解无耗散的纯对流方程时,初始波的能量可以以类似于扩散运动的方式降低。这种方法被称为包含耗散。在某些情况下,有意添加了“人工放散” ,以改善解决方案的数值稳定性特性。
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在计算物理学,数值耗散(也称为“数值扩散”)是指某些副作用,可能发生的结果,数值解的微分方程。用数值近似方法求解无耗散的纯对流方程时,初始波的能量可以以类似于扩散运动的方式降低。这种方法被称为包含耗散。在某些情况下,有意添加“人为放散”以改善解决方案的数值稳定性特性。
 
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=== Mathematics ===
 
=== Mathematics ===
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=== Mathematics ===
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数学
      
A formal, mathematical definition of dissipation, as commonly used in the mathematical study of [[measure-preserving dynamical system]]s, is given in the article ''[[wandering set]]''.
 
A formal, mathematical definition of dissipation, as commonly used in the mathematical study of [[measure-preserving dynamical system]]s, is given in the article ''[[wandering set]]''.
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== Examples ==
      
== Examples ==
 
== Examples ==
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例子
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=== In hydraulic engineering ===
 
=== In hydraulic engineering ===
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=== In hydraulic engineering ===
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水利工程
      
Dissipation is the process of converting mechanical energy of downward-flowing water into thermal and acoustical energy. Various devices are designed in stream beds to reduce the kinetic energy of flowing waters to reduce their [[erosion|erosive potential]] on banks and [[stream bed|river bottoms]]. Very often, these devices look like small [[waterfall]]s or [[waterfall#Types|cascades]], where water flows vertically or over [[riprap]] to lose some of its [[kinetic energy]].
 
Dissipation is the process of converting mechanical energy of downward-flowing water into thermal and acoustical energy. Various devices are designed in stream beds to reduce the kinetic energy of flowing waters to reduce their [[erosion|erosive potential]] on banks and [[stream bed|river bottoms]]. Very often, these devices look like small [[waterfall]]s or [[waterfall#Types|cascades]], where water flows vertically or over [[riprap]] to lose some of its [[kinetic energy]].
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Dissipation is the process of converting mechanical energy of downward-flowing water into thermal and acoustical energy. Various devices are designed in stream beds to reduce the kinetic energy of flowing waters to reduce their erosive potential on banks and river bottoms. Very often, these devices look like small waterfalls or cascades, where water flows vertically or over riprap to lose some of its kinetic energy.
 
Dissipation is the process of converting mechanical energy of downward-flowing water into thermal and acoustical energy. Various devices are designed in stream beds to reduce the kinetic energy of flowing waters to reduce their erosive potential on banks and river bottoms. Very often, these devices look like small waterfalls or cascades, where water flows vertically or over riprap to lose some of its kinetic energy.
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耗散是将向下流动的水的机械能转化为热能和声能的过程。在河床上设计了各种装置,以降低流动水的动能,减少它们对河岸和河底的侵蚀潜力。通常情况下,这些装置看起来像小瀑布或瀑布,水垂直流动或越过抛石,失去一些动能。
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耗散是将向下流动的水的机械能转化为热能和声能的过程。在河床上设计了各种装置,以降低流动水的动能,减少它们对河岸和河底的侵蚀潜力。很多时候,这些装置看起来像小瀑布或瀑布,水流垂直流动或越过抛石,失去一些动能。
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=== Irreversible processes ===
      
=== Irreversible processes ===
 
=== Irreversible processes ===
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不可逆过程
      
Important examples of irreversible processes are:  
 
Important examples of irreversible processes are:  
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=== Waves or oscillations ===
      
=== Waves or oscillations ===
 
=== Waves or oscillations ===
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波浪或振荡
      
[[Wave]]s or [[oscillation]]s, lose [[energy]] over [[time]], typically from [[friction]] or [[turbulence]]. In many cases, the "lost" energy raises the [[temperature]] of the system. For example, a [[wave]] that loses [[amplitude]] is said to dissipate. The precise nature of the effects depends on the nature of the wave: an [[atmospheric wave]], for instance, may dissipate close to the surface due to [[friction]] with the land mass, and at higher levels due to [[radiative cooling]].
 
[[Wave]]s or [[oscillation]]s, lose [[energy]] over [[time]], typically from [[friction]] or [[turbulence]]. In many cases, the "lost" energy raises the [[temperature]] of the system. For example, a [[wave]] that loses [[amplitude]] is said to dissipate. The precise nature of the effects depends on the nature of the wave: an [[atmospheric wave]], for instance, may dissipate close to the surface due to [[friction]] with the land mass, and at higher levels due to [[radiative cooling]].
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Waves or oscillations, lose energy over time, typically from friction or turbulence. In many cases, the "lost" energy raises the temperature of the system. For example, a wave that loses amplitude is said to dissipate. The precise nature of the effects depends on the nature of the wave: an atmospheric wave, for instance, may dissipate close to the surface due to friction with the land mass, and at higher levels due to radiative cooling.
 
Waves or oscillations, lose energy over time, typically from friction or turbulence. In many cases, the "lost" energy raises the temperature of the system. For example, a wave that loses amplitude is said to dissipate. The precise nature of the effects depends on the nature of the wave: an atmospheric wave, for instance, may dissipate close to the surface due to friction with the land mass, and at higher levels due to radiative cooling.
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波浪或振荡,随着时间的推移会失去能量,通常是由于摩擦或紊流。在许多情况下,“损失”的能量提高了系统的温度。例如,失去振幅的波叫做消散波。影响的确切性质取决于波的性质: 例如,一个大气波,可能会因为与陆地的摩擦而接近地表消散,在更高的水平由于辐射冷却。
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波浪或振荡,随着时间的推移会失去能量,通常是由于摩擦或紊流。在许多情况下,“损失”的能量提高了系统的温度。例如,失去振幅的波叫做消散波。影响的确切性质取决于波的性质: 例如,大气波可能由于与陆地质量的摩擦而接近地表消散,由于辐射冷却的缘故而在更高的水平上消散。
 
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== History ==
 
== History ==
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== History ==
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历史
      
{{See also |Timeline of thermodynamics}}
 
{{See also |Timeline of thermodynamics}}
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The concept of dissipation was introduced in the field of thermodynamics by [[William Thomson, 1st Baron Kelvin|William Thomson]] (Lord Kelvin) in 1852.<ref>W. Thomson ''On the universal tendency in nature to the dissipation of mechanical energy'' Philosophical Magazine, Ser. 4, p.&nbsp;304 (1852).</ref> Lord Kelvin deduced that a subset of the above-mentioned irreversible dissipative processes will occur unless a process is governed by a "perfect thermodynamic engine". The processes that Lord Kelvin identified were friction, diffusion, conduction of heat and the absorption of light.
 
The concept of dissipation was introduced in the field of thermodynamics by [[William Thomson, 1st Baron Kelvin|William Thomson]] (Lord Kelvin) in 1852.<ref>W. Thomson ''On the universal tendency in nature to the dissipation of mechanical energy'' Philosophical Magazine, Ser. 4, p.&nbsp;304 (1852).</ref> Lord Kelvin deduced that a subset of the above-mentioned irreversible dissipative processes will occur unless a process is governed by a "perfect thermodynamic engine". The processes that Lord Kelvin identified were friction, diffusion, conduction of heat and the absorption of light.
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耗散的概念是由威廉 · 汤姆森(开尔文勋爵)于1852年在热力学领域提出的。开尔文勋爵推断,上述不可逆耗散过程的一个子集将会发生,除非一个过程被一个“完美的热力学发动机”所支配。开尔文勋爵确定的过程是摩擦、扩散、热传导和光的吸收。
 
耗散的概念是由威廉 · 汤姆森(开尔文勋爵)于1852年在热力学领域提出的。开尔文勋爵推断,上述不可逆耗散过程的一个子集将会发生,除非一个过程被一个“完美的热力学发动机”所支配。开尔文勋爵确定的过程是摩擦、扩散、热传导和光的吸收。
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==See also==
 
==See also==
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==See also==
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参见
      
*[[Entropy production]]
 
*[[Entropy production]]
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*[[Flood control]]
 
*[[Flood control]]
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*[[Principle of maximum entropy]]
 
*[[Principle of maximum entropy]]
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*[[Two-dimensional gas]]
 
*[[Two-dimensional gas]]
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==References==
      
==References==
 
==References==
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参考资料
      
{{Reflist}}
 
{{Reflist}}
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{{Footer energy}}
 
{{Footer energy}}
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