蒸发汽化的基础和使用毕业论文外文翻译.docx

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1、 外文资料C1The basics of steam generation and use1.1 Why an understanding of steam is neededSteam power is fundamental to what is by far the largest sector of the electricity-generating industry and without it the face of contemporary society would be dramatically different from its present one. We woul

2、d be forced to rely on hydro-electric power plant, windmills, batteries, solar cells and fuel cells, all of which are capable of producing only a fraction of the electricity we use.Steam is important, and the safety and efficiency of its generation and use depend on the application of control and in

3、strumentation, often simply referred to as C&I. The objective of this book is to provide a bridge between the discipline of power-plant process engineering and those of electronics, instrumentation and control engineering.I shall start by outlining in this chapter the change of state of water to ste

4、am, followed by an overview of the basic principles of steam generation and use. This seemingly simple subject is extremely complex. This will necessarily be an overview: it does not pretend to be a detailed treatise and at times it will simplify matters and gloss over some details which may even ca

5、use the thermodynamicist or combustion physicist to shudder, but it should be understood that the aim is to provide the C&I engineer with enough understanding of the subject to deal safely with practical control-system design, operational and maintenance problems.1.2 Boiling: the change of state fro

6、m water to steamWhen water is heated its temperature rises in a way that can be detected (for example by a thermometer). The heat gained in this way is called sensible because its effects can be sensed, but at some point the water starts to boil. But here we need to look even deeper into the subject

7、. Exactly what is meant by the expression boiling? To study this we must consider the three basic states of matter: solids, liquids and gases. (A plasma, produced when the atoms in a gas become ionised, is often referred to as the fourth state of matter, but for most practical purposes it is suffici

8、ent to consider only the three basic states.) In its solid state, matter consists of many molecules tightly bound together by attractive forces between them. When the matter absorbs heat the energy levels of its molecules increase and the mean distance between the molecules increases. As more and mo

9、re heat is applied these effects increase until the attractive force between the molecules is eventually overcome and the particles become capable of moving about independently of each other. This change of state from solid to liquid is commonly recognised as melting.As more heat is applied to the l

10、iquid, some of the molecules gain enough energy to escape from the surface, a process called evaporation (whereby a pool of liquid spilled on a surface will gradually disappear). What is happening during the process of evaporation is that some of the molecules are escaping at fairly low temperatures

11、, but as the temperature rises these escapes occur more rapidly and at a certain point the liquid becomes very agitated, with large quantities of bubbles rising to the surface. It is at this time that the liquid is said to start boiling. It is in the process of changing state to a vapour, which is a

12、 fluid in a gaseous state.Let us consider a quantity of water that is contained in an open vessel. Here, the air that blankets the surface exerts a pressure on the surface of the fluid and, as the temperature of the water is raised, enough energy is eventually gained to overcome the blanketing effec

13、t of that pressure and the water starts to change its state into that of a vapour (steam). Further heat added at this stage will not cause any further detectable change in temperature: the energy added is used to change the state of the fluid. Its effect can no longer be sensed by a thermometer, but

14、 it is still there. For this reason it is called latent, rather then sensible, heat. The temperature at which this happens is called the boiling point. At normal atmospheric pressure the boiling point of water is 100 C.If the pressure of the air blanket on top of the water were to be increased, more

15、 energy would have to be introduced it to break free. In other words, the temperature must be raised further to make it boil. To illustrate this point, if the pressure is increased by 10% above its normal atmospheric value, the temperature of the water must be raised to just above 102 C before boili

16、ng occurs.The steam emerging from the boiling liquid is said to be saturated and, for any given pressure, the temperature at which boiling occurs is called the saturation temperature.The information relating to steam at any combination of temperature, pressure and other factors may be found in steam

17、 tables, which are nowadays available in software as well as in the more traditional paper form. These tables were originally published in 1915 by Hugh Longbourne Callendar (1863-1930), a British physicist. Because of advances in knowledge and measurement technology, and as a result of changing unit

18、s of measurement, many different variants of steam tables are today in existence, but they all enable one to look up, for any pressure, the saturation temperature, the heat per unit mass of fluid, the specific volume etc.Understanding steam and the steam tables is essential in many stages of the des

19、ign of power-plant control systems. For example, if a designer needs to compensate a steam-flow measurement for changes in pressure, or to correct for density errors in a water-level measurement, reference to these tables is essential.Another term relating to steam defines the quantity of liquid mix

20、ed in with the vapour. In the UK this is called the dryness fraction (in the USA the term used is steam quality). What this means is that if each kilogram of the mixture contains 0.9 kg of vapour and 0.1 kg of water, the dryness fraction is 0.9.Steam becomes superheated when its temperature is raise

21、d above the saturation temperature corresponding to its pressure. This is achieved by collecting it from the vessel in which the boiling is occurring, leading it away from the liquid through a pipe, and then adding more heat to it. This process adds further energy to the fluid, which improves the ef

22、ficiency of the conversion of heat to electricity.As stated earlier, heat added once the water has started to boil does not cause any further detectable change in temperature. Instead it changes the state of the fluid. Once the steam has formed, heat added to it contributes to the total heat of the

23、vapour. This is the sensible heat plus the latent heat plus the heat used in increasing the temperature of each kilogram of the fluid through the number of degrees of superheat to which it has been raised.In a power plant, a major objective is the conversion of energy locked up in the input fuel int

24、o either usable heat or electricity. In the interests of economics and the environment it is important to obtain the highest to the water to enable possible level of efficiency in this conversion process. As we have already seen, the greatest efficiency is obtained by maximising the energy level of

25、the steam at the point of delivery to the next stage of the process. When as much energy as possible has been abstracted from the steam, the fluid reverts to the form of cold water, which is then warmed and treated to remove any air which may have become entrained in it before it is finally returned

26、 to the boiler for re-use.1.3 The nature of steamAs stated in the Preface, the boilers and steam-generators that are the subject of this book provide steam to users such as industrial plant, or housing and other complexes, or to drive turbines that are the prime movers for electrical generators. For

27、 the purposes of this book, such processes are grouped together under the generic name power plant. In all these applications the steam is produced by applying heat to water until it boils, and before we embark on our study of power-plant C&I we must understand the mechanisms involved in this proces

28、s and the nature of steam itself.First, we must pause to consider some basic thermodynamic processes. Two of these are the Carnot and Rankine cycles, and although the C&I engineer may not make use of these directly, it is nevertheless useful to have a basic understanding of what they are how they op

29、erate.1.3.1 The Carnot cycleThe primary function of a power plant is to convert into electricity the energy locked up in some form of fuel resource. In spite of many attempts, it has not proved possible to generate electricity in large quantities from the direct conversion of the energy contained in

30、 a fossil fuel (or even a nuclear fuel) without the use of a medium that acts as an intermediary. Solar cells and fuel cells may one day achieve this aim on a scale large enough to make an impact on fossil-fuel utilisation, but at present such plants are confined to small-scale applications. The wat

31、er turbines of hydro-electric plants are capable of generating large quantities of electricity, but such plants are necessarily restricted to areas where they are plentiful supplies of water at heights sufficient for use by these machines.Therefore, if one wishes to obtain large quantities of electr

32、icity from a fossil fuel or from a nuclear reaction it is necessary to first release the energy that is available within that resource and then to transfer it to a generator, and this process necessitates the use of a medium to convey the energy from source to destination. Furthermore, it is necessa

33、ry to employ a medium that is readily available and which can be used with relative safety and efficiency. On plant Earth, water is, at least in general, a plentiful and cheap medium for effecting such transfers. With the development of technology during the twentieth century other possibilities hav

34、e been considered, such as the use of mercury, but except for applications such as spacecraft where entirely new sets of limitations and conditions apply, none of these has reached active use, and steam is universally used in power stations.Figure A1Carnot framed one of the two laws of thermodynamic

35、s. The first, Joules law, had related mechanical energy to work: Carnots law defined the temperature relations applying to the conversion of heat energy into mechanical energy. He saw that if this process were to be made reversible, heat could be converted into work and then extracted and re-used to

36、 make a closed loop. In his concept (Figure A1), a piston moves freely without encountering any friction inside a cylinder made of some perfectly insulating material. The piston is driven by a working fluid. The cylinder has a head at one end that can be switched at will from being a perfect conduct

37、or to being a perfect insulator. Outside the cylinder are two bodies, one of which can deliver heat without its own temperature ( T1 ) falling, the other being a bottomless cold sink at a temperature (T2) which is also constant.The operation of the system is shown graphically in figure A2, which sho

38、ws the pressure/volume relationship of the fluid in the cylinder over the whole cycle. As the process is a repeating cycle its operation can be studied from any convenient starting point, and we shall begin at the point A, where the cylinder head (at this time assumed to be a perfect conductor of he

39、at), allows heat from the hot source to enter the cylinder. The result is that the medium begins to expand, and if it is allowed to expand freely, Boyles law (which states that at any temperature the relationship between pressure and volume is constant) dictates that the temperature will not rise, b

40、ut will stay at its initial temperature (Tl). This is called isothermal expansion.Figure A2When the pressure and volume of the medium have reached the values at point B, the cylinder head is switched from being a perfect conductor to being a perfect insulator and the medium allowed to continue its e

41、xpansion with no heat being gained or lost. This is known as adiabatic expansion. When the pressure and volume of the medium reach the values at point C, the cylinder head is switched back to being a perfect conductor, but the external heat source is removed and replaced by the heat sink. The piston

42、 is driven towards the head, compressing the medium. Heat flows through the head to the heat sink and when the temperature of the medium reaches that of the heat sink (at point D), the cylinder head is once again switched to become a perfect insulator and the medium is compressed until it reaches it

43、s starting conditions of pressure and temperature.The cycle is then complete, having taken in and rejected heat while doing external work.1.3.2 The Rankine cycleThe Carnot cycle postulates a cylinder with perfectly insulating walls and a head which can be switched at will from Being a conductor to b

44、eing an insulator. Even with modifications to enable it to operate in a world where such things are not obtainable, it would have probably remained a scientific concept with no practical application, had not a Scottish professor of engineering, William Rankine, proposed a modification to it at the b

45、eginning of the twentieth century I. The concepts that Rankine developed form the basis of all thermal power plants in use today. Even todays combined-cycle power plants use his cycle for one of the two phases of their operation.Figure A3 illustrates the principle of the Rankine cycle. Starting at p

46、oint A again, the source of heat is applied to expand the medium, this time at a constant pressure, to point B, after which adiabatic expansion is again made to occur until the medium reaches the conditions at point C. From here, the volume of the medium is reduced, at a constant pressure, until it

47、reaches point D, when it is compressed back to its initial conditions.Figure A3中文翻译C2蒸发汽化的基础和使用1.1 为何需要了解蒸汽对于目前为止最大的发电工业部门来说，蒸汽动力是最为基础性的。若没有蒸汽动力，社会的样子将会变得和现在大为不同。我们将不得已的去依靠水力发电厂、风车、电池、太阳能蓄电池和燃料电池，这些方法只能为我们平日用电提供很小的一部分。蒸汽是很重要的，产生和使用蒸汽的安全与效率取决于怎样控制和应用仪表，在术语中通常被简写成C&I（控制和仪表）。此书旨在在发电厂的工程规程和电子学、仪器仪表以及控制工

48、程之间架设一座桥梁。作为开篇，我将在本章大体描述由水到蒸汽的形态变化，然后将叙述蒸汽产生和使用的基本原则的概述。这看似简单的课题实际上却极为复杂。这里，我们有必要做一个概述：这本书不是内容详尽的论文，有的时候甚至会掩盖一些细节，而这些细节将会使热力学家和燃烧物理学家都为之一震。但我们应该了解，这本书的目的是为了使控制仪表工程师充分理解这一课题，从而可以安全的处理实用控制系统设计、运作、维护等方面的问题。，1.2沸腾：水到蒸汽的状态变化当水被加热时，其温度变化能通过某种途径被察觉（例如用温度计）。通过这种方式得到的热量因为在某时水开始沸腾时其效果可被察觉，因而被称为感热。然而，我们还需要更深的了

49、解。“沸腾”究竟是什么含义？在深入了解之前，我们必须考虑到物质的三种状态：固态，液态，气态。（当气体中的原子被电离时所产生的等离子气体经常被认为是物质的第四种状态，但在实际应用中，只需考虑以上三种状态）固态，物质由分子通过分子间的吸引力紧紧地靠在一起。当物质吸收热量，分子的能量升级并且使得分子之间的间隙增大。当越来越多的能量被吸收，这种效果就会加剧，粒子之间相互脱离。这种由固态到液态的状态变化通常被称之为熔化。当液体吸收了更多的热量时，一些分子获得了足够多的能量而从表面脱离，这个过程被称为蒸发（凭此洒在地面的水会逐渐的消失）在蒸发的过程中，一些分子是在相当低的温度下脱离的，然而随着温度的上升，分子更加迅速的脱离，并且在某一温度上液体内部变得非常剧烈，大量的气泡向液体表面升起。在这时我们称液体开始沸腾。这个过程是变为蒸汽的过程，也就是液体处于汽化状态。让我们试想大量的水装在一个敞开的容器内。液体表面的空气对液体施加了一定的压力，随着液体温度的上升，便会有足够的能量使得表面的分子挣脱出去，水这时开始改变自身的状态，变成蒸汽。在此条件下获得更多的热量将不会