附录A 译文
变压器
1. 介绍
要从远端发电厂送出电能，必须应用高压输电。因为最终的负荷，在一些点高电压必须降低。变压器能使电力系统各个部分运行在电压不同的等级。本文我们讨论的原则和电力变压器的应用。
2. 双绕组变压器
变压器的最简单形式包括两个磁通相互耦合的固定线圈。两个线圈之所以相互耦合，是因为它们连接着共同的磁通。
在电力应用中，使用层式铁芯变压器(本文中提到的)。变压器是高效率的，因为它没有旋转损失，因此在电压等级转换的过程中，能量损失比较少。典型的效率范围在92到99%，上限值适用于大功率变压器。
从交流电源流入电流的一侧被称为变压器的一次侧绕组或者是原边。它在铁圈中建立了磁通φ，它的幅值和方向都会发生周期性的变化。磁通连接的第二个绕组被称为变压器的二次侧绕组或者是副边。磁通是变化的；因此依据楞次定律，电磁感应在二次侧产生了电压。变压器在原边接收电能的同时也在向副边所带的负荷输送电能。这就是变压器的作用。
3. 变压器的工作原理
当二次侧电路开路是，即使原边被施以正弦电压V p，也是没有能量转移的。外加电压在一次侧绕组中产生一个小电流Iθ。这个空载电流有两项功能：（1）在铁芯中产生电磁通，该磁通在零和 φm之间做正弦变化，φm是铁芯磁通的最大值；（2）它的一个分量说明了铁芯中的涡流和磁滞损耗。这两种相关的损耗被称为铁芯损耗。
变压器空载电流Iθ一般大约只有满载电流的2%—5%。因为在空载时，原边绕组中的铁芯相当于一个很大的电抗，空载电流的相位大约将滞后于原边电压相位90o。显然可见电流分量I m= I0sinθ0，被称做励磁电流，它在相位上滞后
于原边电压V P 90o。就是这个分量在铁芯中建立了磁通；因此磁通φ与I m 同相。
第二个分量I e =I 0sin θ0，与原边电压同相。这个电流分量向铁芯提供用于损耗的电流。两个相量的分量和代表空载电流，即I 0 = I m + I e
应注意的是空载电流是畸变和非正弦形的。这种情况是非线性铁芯材料造成的。
如果假定变压器中没有其他的电能损耗一次侧的感应电动势E p 和二次侧的感应电压E s 可以表示出来。因为一次侧绕组中的磁通会通过二次绕组，依据法拉第电磁感应定律，二次侧绕组中将产生一个电动势E ，即E=N Δφ/Δt 。相同的磁通会通过原边自身，产生一个电动势E p 。正如前文中讨论到的，所产生的电压必定滞后于磁通90o，因此，它于施加的电压有180o的相位差。因为没有电流流过二次侧绕组，E s =V s 。一次侧空载电流很小，仅为满载电流的百分之几。因此原边电压很小，并且V p 的值近乎等于E p 。原边的电压和它产生的磁通波形是正弦形的；因此产生电动势E p 和E s 的值是做正弦变化的。产生电压的平均值如下
E avg = turns×给定时间内磁通变化量
给定时间
即是法拉第定律在瞬时时间里的应用。它遵循
E avg = N 21/(2)m f = 4fN φm
其中N 是指线圈的匝数。从交流电原理可知，有效值是一个正弦波，其值为平均电压的1.11倍；因此
E = 4.44fN φm
因为一次侧绕组和二次侧绕组的磁通相等，所以绕组中每匝的电压也相同。因此
E p = 4.44fN p φm
并且
E s = 4.44fN s φm
其中N p 和E s 是一次侧绕组和二次侧绕组的匝数。一次侧和二次侧电压增长的比
率称做变比。用字母a 来表示这个比率，如下式a = p
s E E = p s N N
假设变压器输出电能等于其输入电能——这个假设适用于高效率的变压器。实际上我们是考虑一台理想状态下的变压器；这意味着它没有任何损耗。因此
P m = P out
或者
V p I p × primary PF = V s I s × secondary PF
这里PF 代表功率因素。在上面公式中一次侧和二次侧的功率因素是相等的；因此
V p I p = V s I s
从上式我们可以得知
p
s V V = p s I I ≌ p s E E ≌ a
它表明端电压比等于匝数比，换句话说，一次侧和二次侧电流比与匝数比成反比。匝数比可以衡量二次侧电压相对于一次恻电压是升高或者是降低。为了计算电压，我们需要更多数据。
终端电压的比率变化有些根据负载和它的功率因素。实际上, 变比从标识牌数据获得, 列出在满载情况下原边和副边电压。
当副边电压V s 相对于原边电压减小时，这个变压器就叫做降压变压器。如果这个电压是升高的，它就是一个升压变压器。在一个降压变压器中传输变比a 远大于1(a>1.0)，同样的，一个升压变压器的变比小于1(a<1.0)。当a=1时，变压器的二次侧电压就等于起一次侧电压。这是一种特殊类型的变压器，可被应用于当一次侧和二次侧需要相互绝缘以维持相同的电压等级的状况下。因此，我们把这种类型的变压器称为绝缘型变压器。
显然，铁芯中的电磁通形成了连接原边和副边的回路。在第四部分我们会了解到当变压器带负荷运行时一次侧绕组电流是如何随着二次侧负荷电流变化而变化的。
从电源侧来看变压器，其阻抗可认为等于V p / I p 。从等式 p
s V V = p s I I ≌ p s E E ≌
a 中我们可知V p = aV s
并且I p = I s /a 。根据V s 和I s ，可得V p 和I p 的比例是
p
p V I = /s s aV I a = 2s s a V I
但是V s / I s 负荷阻抗Z L ，因此我们可以这样表示
Z m (primary) = a 2Z L
这个等式表明二次侧连接的阻抗折算到电源侧，其值为原来的a 2倍。我们把这种折算方式称为负载阻抗向一次侧的折算。这个公式应用于变压器的阻抗匹配。
4. 有载情况下的变压器
一次侧电压和二次侧电压有着相同的极性，一般习惯上用点记号表示。如果点号同在线圈的上端，就意味着它们的极性相同。因此当二次侧连接着一个负载时，在瞬间就有一个负荷电流沿着这个方向产生。换句话说，极性的标注可以表明当电流流过两侧的线圈时，线圈中的磁动势会增加。
因为二次侧电压的大小取决于铁芯磁通大小φ0，所以很显然当正常情况下负载电势E s 没有变化时，二次侧电压也不会有明显的变化。当变压器带负荷运行时，将有电流I s 流过二次侧，因为E s 产生的感应电动势相当于一个电压源。二次侧电流产生的磁动势N s I s 会产生一个励磁。这个磁通的方向在任何一个时刻都和主磁通反向。当然，这是楞次定律的体现。因此，N s I s 所产生的磁动势会使主磁通φ0减小。这意味着一次侧线圈中的磁通减少，因而它的电压E p 将会增大。感应电压的减小将使外施电压和感应电动势之间的差值更大，它将使初级线圈中流过更大的电流。初级线圈中的电流I p 的增大，意味着前面所说明的两个条件都满足：（1）输出功率将随着输出功率的增加而增加（2）初级线圈中的磁动势将增加，以此来抵消二次侧中的磁动势减小磁通的趋势。
总的来说，变压器为了保持磁通是常数，对磁通变化的响应是瞬时的。更重要的是，在空载和满载时，主磁通φ0的降落是很少的（一般在）1至3%。其需要的条件是E 降落很多来使电流I p 增加。
在一次侧，电流I p ’
在一次侧流过以平衡I s 产生的影响。它的磁动势N p I p ’
只停留在一次侧。因为铁芯的磁通φ0保持不变，变压器空载时空载电流I0必定会为其提供能量。故一次侧电流I p是电流I p’与I0’的和。
因为空载电流相对较小，那么一次侧的安匝数与二次侧的安匝数相等的假设是成立的。因为在这种状况下铁芯的磁通是恒定的。因此我们仍旧可以认定空载电流I0相对于满载电流是极其小的。
当一个电流流过二次侧绕组，它的磁动势（N s I s）将产生一个磁通，于空载电流I0产生的磁通φ0不同，它只停留在二次侧绕组中。因为这个磁通不流过一次侧绕组，所以它不是一个公共磁通。
另外，流过一次侧绕组的负载电流只在一次侧绕组中产生磁通，这个磁通被称为一次侧的漏磁。二次侧漏磁将使电压增大以保持两侧电压的平衡。一次侧漏磁也一样。因此，这两个增大的电压具有电压降的性质，总称为漏电抗电压降。另外，两侧绕组同样具有阻抗，这也将产生一个电阻压降。把这些附加的电压降也考虑在内，这样一个实际的变压器的等值电路图就完成了。由于分支励磁体现在电流里，为了分析我们可以将它忽略。这就符我们前面计算中可以忽略空载电流的假设。这证明了它对我们分析变压器时所产生的影响微乎其微。因为电压降与负载电流成比例关系，这就意味着空载情况下一次侧和二次侧绕组的电压降都为零。
附录B 外文原文
TRANSFORMER
1. INTRODUCTION
The high-voltage transmission was need for the case electrical power is to be provided at considerable distance from a generating station. At some point this high voltage must be reduced, because ultimately is must supply a load. The transformer makes it possible for various parts of a power system to operate at different voltage levels. In this paper we discuss power transformer principles and applications.
2. TOW-WINDING TRANSFORMERS
A transformer in its simplest form consists of two stationary coils coupled by a mutual magnetic flux. The coils are said to be mutually coupled because they link a common flux.
In power applications, laminated steel core transformers (to which this paper is restricted) are used. Transformers are efficient because the rotational losses normally associated with rotating machine are absent, so relatively little power is lost when transforming power from one voltage level to another. Typical efficiencies are in the range 92 to 99%, the higher values applying to the larger power transformers.
The current flowing in the coil connected to the ac source is called the primary winding or simply the primary. It sets up the flux φ in the core, which varies periodically both in magnitude and direction. The flux links the second coil, called the secondary winding or simply secondary. The flux is changing; therefore, it induces a voltage in the secondary by electromagnetic induction in accordance with Lenz’s law. Thus the primary receives its power from the source while the secondary supplies this power to the load. This action is known as transformer action.
3. TRANSFORMER PRINCIPLES
When a sinusoidal voltage V p is applied to the primary with the secondary open-circuited, there will be no energy transfer. The impressed voltage causes a small current Iθ to flow in the primary winding. This no-load current has two functions: (1) it produces the magnetic flux in the core, which varies sinusoidally between zero and φm, where φm is the maximum value of the core flux; and (2) it provides a component to account for the hysteresis and eddy current losses in the core. There combined losses are normally referred to as the core losses.
The no-load current Iθis usually few percent of the rated full-load current of the transformer (about 2 to 5%). Since at no-load the primary winding acts as a large reactance due to the iron core, the no-load current will lag the primary voltage by nearly 90o. It is readily seen that the current component I m= I0sinθ0, called the magnetizing current, is 90oin phase behind the primary voltage V P. It is this component that sets up the flux in the core; φ is therefore in phase with I m.
The second component, I e=I0sinθ0, is in phase with the primary voltage. It is the current component that supplies the core losses. The phasor sum of these two components represents the no-load current, or
I0 = I m+ I e
It should be noted that the no-load current is distortes and nonsinusoidal. This is the result of the nonlinear behavior of the core material.
If it is assumed that there are no other losses in the transformer, the induced voltage In the primary , E p and that in the secondary , E s can be shown. Since the magnetic flux set up by the primary winding ，there will be an induced EMF E in the secondary winding in accordance with Faraday’s law, namely , E=NΔφ/Δt. This same flux also links the primary itself, inducing in it an EMF, E p . As discussed earlier, the induced voltage must lag the flux by 90o, therefore, they are 180o out of phase with the applied voltage. Since no current flows in the secondary winding, E s =V s . The no-load primary current I 0 is small, a few percent of full-load current. Thus the voltage in the primary is small and V p is nearly equal to E p . The primary voltage and the resulting flux are sinusoidal; thus the induced quantities E p and E s vary as a sine function. The average value of the induced voltage given by
E avg = turns× change in flux in a given time
given time
which is Faraday’s law applied to a finite time interval. It follows that
E avg = N 21/(2)m
f = 4fNφm
which N is the number of turns on the winding. Form ac circuit theory , the effective or root-mean-square (rms) voltage for a sine wave is 1.11 times the average voltage; thus
E = 4.44fNφm
Since the same flux links with the primary and secondary windings, the voltage per turn in each winding is the same. Hence
E p = 4.44fN p φm
and
E s = 4.44fN s φm
where E p and Es are the number of turn on the primary and secondary windings, respectively . The ratio of primary to secondary induced voltage is called the transformation ratio. Denoting this ratio by a, it is seen that
a = p
s E E = p s N N
Assume that the output power of a transformer equals its input power, not a bad sumption in practice considering the high efficiencies. What we really are saying is that we are dealing with an ideal transformer; that is, it has no losses. Thus
P m = P out
or
V p I p × primary PF = V s I s × secondary PF
where PF is the power factor. For the above-stated assumption it means that the power factor on primary and secondary sides are equal; therefore
V p I p = V s I s from which is obtained
p
s V V = p s I I ≌ p s E E ≌ a
It shows that as an approximation the terminal voltage ratio equals the turns ratio. The primary and secondary current, on the other hand, are inversely related to the turns ratio. The turns ratio gives a measure of how much the secondary voltage is raised or lowered in relation to the primary voltage. To calculate the voltage regulation, we need more information.
The ratio of the terminal voltage varies somewhat depending on the load and its power factor. In practice, the transformation ratio is obtained from the nameplate data, which list the primary and secondary voltage under full-load condition.
When the secondary voltage V s is reduced compared to the primary voltage, the transformation is said to be a step-down transformer: conversely, if this voltage is raised, it is called a step-up transformer. In a step-down transformer the transformation ratio a is greater than unity (a>1.0), while for a step-up transformer it is smaller than unity (a<1.0). In the event that a=1, the transformer secondary voltage equals the primary voltage. This is a special type of transformer used in instances where electrical isolation is required between the primary and secondary circuit while maintaining the same voltage level. Therefore, this transformer is generally knows as an isolation transformer.
As is apparent, it is the magnetic flux in the core that forms the connecting link between primary and secondary circuit. In section 4 it is shown how the primary winding current adjusts itself to the secondary load current when the transformer supplies a load.
Looking into the transformer terminals from the source, an impedance is seen which by definition equals V p / I p . From p
s V V = p s I I ≌ p s E E ≌ a , we have V p = aV s
and I p = I s /a.In terms of V s and I s the ratio of V p to I p is
p
p V I = /s s aV I a = 2s s a V I
But V s / I s is the load impedance Z L thus we can say that
Z m (primary) = a 2Z L
This equation tells us that when an impedance is connected to the secondary side, it appears from the source as an impedance having a magnitude that is a 2 times its actual value. We say that the load impedance is reflected or referred to the primary . It is this property of transformers that is used in impedance-matching applications.
4. TRANSFORMERS UNDER LOAD
The primary and secondary voltages shown have similar polarities, as indicated by the “dot -making” convention. The dots near the upper ends of t he windings have the same meaning as in circuit theory; the marked terminals have the same polarity . Thus when a load is connected to the secondary , the instantaneous load current is in the direction shown. In other words, the polarity markings signify that when positive current enters both windings at the marked terminals, the MMFs of the two windings add.
Since the secondary voltage depends on the core flux φ0, it must be clear that the flux should not change appreciably if E s is to remain essentially constant under normal loading conditions. With the load connected, a current I s will flow in the secondary circuit, because the induced EMF E s will act as a voltage source. The secondary current produces an MMF N s I s that creates a flux. This flux has such a direction that at any instant in time it opposes the main flux that created it in the first
place. Of course, this is Lenz’s law in action. Thus the MMF represented by N s I s tends to reduce the core flux φ0. This means that the flux linking the primary winding reduces and consequently the primary induced voltage E p, This reduction in induced voltage causes a greater difference between the impressed voltage and the counter induced EMF, thereby allowing more current to flow in the primary. The fact that primary current I p increases means that the two conditions stated earlier are fulfilled: (1) the power input increases to match the power output, and (2) the primary MMF increases to offset the tendency of the secondary MMF to reduce the flux.
In general, it will be found that the transformer reacts almost instantaneously to keep the resultant core flux essentially constant. Moreover, the core flux φ0 drops very slightly between n o load and full load (about 1 to 3%), a necessary condition if E p is to fall sufficiently to allow an increase in I p.
On the primary side, I p’is the current that flows in the primary to balance the demagnetizing effect of I s. Its MMF N p I p’sets up a flux linking the primary only. Since the core flux φ0 remains constant. I0 must be the same current that energizes the transformer at no load. The primary current I p is therefore the sum of the current I p’and I0.
Because the no-load current is relatively small, it is correct to assume that the primary ampere-turns equal the secondary ampere-turns, since it is under this condition that the core flux is essentially constant. Thus we will assume that I0is negligible, as it is only a small component of the full-load current.
When a current flows in the secondary winding, the resulting MMF (N s I s) creates a separate flux, apart from the flux φ0produced by I0, which links the secondary winding only. This flux does no link with the primary winding and is therefore not a mutual flux.
In addition, the load current that flows through the primary winding creates a flux that links with the primary winding only; it is called the primary leakage flux. The secondary- leakage flux gives rise to an induced voltage that is not counter balanced by an equivalent induced voltage in the primary. Similarly, the volta ge induced in the primary is not counterbalanced in the secondary winding. Consequently,
these two induced voltages behave like voltage drops, generally called leakage reactance voltage drops. Furthermore, each winding has some resistance, which produces a resistive voltage drop. When taken into account, these additional voltage drops would complete the equivalent circuit diagram of a practical transformer. Note that the magnetizing branch is shown in this circuit, which for our purposes will be disregarded. This follows our earlier assumption that the no-load current is assumed negligible in our calculations. This is further justified in that it is rarely necessary to predict transformer performance to such accuracies. Since the voltage drops are all directly proportional to the load current, it means that at no-load conditions there will be no voltage drops in either winding.
中英文对照资料外文翻译文献 附件1：外文资料翻译译文 传感器新技术的发展 传感器是一种能将物理量、化学量、生物量等转换成电信号的器件。输出信号有不同形式，如电压、电流、频率、脉冲等，能满足信息传输、处理、记录、显示、控制要求，是自动检测系统和自动控制系统中不可缺少的元件。如果把计算机比作大脑，那么传感器则相当于五官，传感器能正确感受被测量并转换成相应输出量，对系统的质量起决定性作用。自动化程度越高，系统对传感器要求越高。在今天的信息时代里，信息产业包括信息采集、传输、处理三部分，即传感技术、通信技术、计算机技术。现代的计算机技术和通信技术由于超大规模集成电路的飞速发展，而已经充分发达后，不仅对传感器的精度、可靠性、响应速度、获取的信息量要求越来越高，还要求其成本低廉且使用方便。显然传统传感器因功能、特性、体积、成本等已难以满足而逐渐被淘汰。世界许多发达国家都在加快对传感器新技术的研究与开发，并且都已取得极大的突破。如今传感器新技术的发展，主要有以下几个方面： 利用物理现象、化学反应、生物效应作为传感器原理，所以研究发现新现象与新效应是传感器技术发展的重要工作，是研究开发新型传感器的基础。日本夏普公司利用超导技术研制成功高温超导磁性传感器，是传感器技术的重大突破，其灵敏度高，仅次于超导量子干涉器件。它的制造工艺远比超导量子干涉器件简单。可用于磁成像技术，有广泛推广价值。 利用抗体和抗原在电极表面上相遇复合时，会引起电极电位的变化，利用这一现象可制出免疫传感器。用这种抗体制成的免疫传感器可对某生物体内是否有这种抗原作检查。如用肝炎病毒抗体可检查某人是否患有肝炎，起到快速、准确作用。美国加州大学巳研制出这类传感器。 传感器材料是传感器技术的重要基础，由于材料科学进步，人们可制造出各种新型传感器。例如用高分子聚合物薄膜制成温度传感器；光导纤维能制成压力、流量、温度、位移等多种传感器；用陶瓷制成压力传感器。
变频器外文翻译文献 (文档含中英文对照即英文原文和中文翻译)
外文: Converter reference design (1)Converter Selection: Selection to determine the frequency converter when the following points: 1) The purpose of a variable frequency; constant pressure to control or constant current control. 2) the load converter types such as leaves or pump volume pumps, with special attention to load the performance curve, the performance curve of the decision of the ways and means. 3) the frequency converter and load matching Voltage match: a rated voltage converter with a rated voltage line with the load. Current matches: ordinary pump, the rated current inverter and motor rated current match. For special load such as deep-water pumps, and so on need to refer to the electrical performance parameters to determine the most current inverter current and Guozainengli. Torque match: in this case constant torque load or slow down when the device may have occurred. 4) the use of high-speed motor drive inverter, because of the high-speed motor, anti-small, high harmonics lead to increased output current value increases. So for high-speed motor inverter Selection, its capacity to be slightly larger than the ordinary motor selection. 5) If the frequency converter to a long cable run, this time to take measures to curb the long cable to the impact of capacitive coupling, inadequate efforts to avoid converter, so in this case, the drive to enlarge the capacity of a file or the converter Output installed output reactor. 6) For the application of some special occasions, such as high temperatures, high altitude, at this time would cause the down converter capacity, the drive to enlarge the capacity of a block.
译自<<科技英语>> 变压器 1. 介绍 要从远端发电厂送出电能，必须应用高压输电。因为最终的负荷，在一些点高电压必须降低。变压器能使电力系统各个部分运行在电压不同的等级。本文我们讨论的原则和电力变压器的应用。 2. 双绕组变压器 变压器的最简单形式包括两个磁通相互耦合的固定线圈。两个线圈之所以相互耦合，是因为它们连接着共同的磁通。 在电力应用中，使用层式铁芯变压器(本文中提到的)。变压器是高效率的，因为它没有旋转损失，因此在电压等级转换的过程中，能量损失比较少。典型的效率范围在92到99%，上限值适用于大功率变压器。 从交流电源流入电流的一侧被称为变压器的一次侧绕组或者是原边。它在铁圈中建立了磁通φ，它的幅值和方向都会发生周期性的变化。磁通连接的第二个绕组被称为变压器的二次侧绕组或者是副边。磁通是变化的；因此依据楞次定律，电磁感应在二次侧产生了电压。变压器在原边接收电能的同时也在向副边所带的负荷输送电能。这就是变压器的作用。 3. 变压器的工作原理 当二次侧电路开路是，即使原边被施以正弦电压V p，也是没有能量转移的。外加电压在一次侧绕组中产生一个小电流Iθ。这个空载电流有两项功能：（1）在铁芯中产生电磁通，该磁通在零和 φm之间做正弦变化，φm是铁芯磁通的最大值；（2）它的一个分量说明了铁芯中的涡流和磁滞损耗。这两种相关的损耗被称为铁芯损耗。 变压器空载电流Iθ一般大约只有满载电流的2%—5%。因为在空载时，原边绕组中的铁芯相当于一个很大的电抗，空载电流的相位大约将滞后于原边电压相位90o。显然可见电流分量I m= I0sinθ0，被称做励磁电流，它在相位上滞后于原边电压V P 90o。就是这个分量在铁芯中建立了磁通；因此磁通φ与I m同相。 第二个分量I e=I0sinθ0，与原边电压同相。这个电流分量向铁芯提供用于损耗的电流。两个相量的分量和代表空载电流，即 I0 = I m+ I e 应注意的是空载电流是畸变和非正弦形的。这种情况是非线性铁芯材料造成的。 如果假定变压器中没有其他的电能损耗一次侧的感应电动势E p和二次侧的感
中英文资料对照外文翻译 基于网络共享的无线传感网络设计 摘要：无线传感器网络是近年来的一种新兴发展技术，它在环境监测、农业和公众健康等方面有着广泛的应用。在发展中国家，无线传感器网络技术是一种常用的技术模型。由于无线传感网络的在线监测和高效率的网络传送，使其具有很大的发展前景，然而无线传感网络的发展仍然面临着很大的挑战。其主要挑战包括传感器的可携性、快速性。我们首先讨论了传感器网络的可行性然后描述在解决各种技术性挑战时传感器应产生的便携性。我们还讨论了关于孟加拉国和加利 尼亚州基于无线传感网络的水质的开发和监测。 关键词：无线传感网络、在线监测 1.简介 无线传感器网络，是计算机设备和传感器之间的桥梁，在公共卫生、环境和农业等领域发挥着巨大的作用。一个单一的设备应该有一个处理器，一个无线电和多个传感器。当这些设备在一个领域部署时，传感装置测量这一领域的特殊环境。然后将监测到的数据通过无线电进行传输，再由计算机进行数据分析。这样，无线传感器网络可以对环境中各种变化进行详细的观察。无线传感器网络是能够测量各种现象如在水中的污染物含量，水灌溉流量。比如，最近发生的污染涌流进中国松花江，而松花江又是饮用水的主要来源。通过测定水流量和速度，通过传感器对江水进行实时监测，就能够确定污染桶的数量和流动方向。 不幸的是，人们只是在资源相对丰富这个条件下做文章，无线传感器网络的潜力在很大程度上仍未开发，费用对无线传感器网络是几个主要障碍之一，阻止了其更广阔的发展前景。许多无线传感器网络组件正在趋于便宜化（例如有关计算能力的组件），而传感器本身仍是最昂贵的。正如在在文献[5]中所指出的，成功的技术依赖于
Constant pressure water supply frequency changer The transistor frequency changer not only overcame has formerly exchanged velocity modulation many shortcomings, moreover the velocity modulation performance might compare favorably with the direct current motor velocity modulation performance. The three-phase asynchronous motor has the service to be convenient, merit and so on price small advantage, power and rotational speed adapt breadth, its frequency conversion velocity modulation technology in the miniaturization, the low cost and the redundant reliable aspect holds the obvious superiority. To the end of the 80's, the alternating current machine frequency conversion velocity modulation technology rapidly develops into a mature technology, it will supply the alternating current machine the labor frequency alternating current supply to turn direct current after the diode rectification, again by component and so on IGBT or GTR module counter will turn the alternating current supply which the frequency might move, will drive the electrical machinery by this power source to move under the speed change condition, and automatic suitable strain load condition. After it changed in the traditional industry the electrical machinery to start only can by the rated power, decide the rotational speed the sole movement way, thus achieved the energy conservation goal. The modern frequency conversion velocity modulation technology applies in the electric power water pump water supply system. Because the frequency conversion velocity modulation has the velocity modula -tion the physical characteristics well, efficiency high, velocity modulation scope -wide, precision high, adjusting character curve smooth, may continual realize, the steady velocity modulation, the volume small, the maintenance simple is conven -ient, the automated level higher a series of prominent merits but time people's favor. When it applies especially in the air blower, the water pump and so on the large capacity load, may obtain the energy conservation effect which other velocity modulation ways is unable to compare. The frequency conversion velocity modulation system main equipment is provides the frequency conversion power source the frequency changer, the frequency changer may divide into exchange - direct current - to exchange the frequency changer and the exchange - exchan
附录 INTERNATIONAL STANDARD POWER TRANSFORMERS 1. Scope and service conditions 1.1 Scope This part of international Standard IEC60076 applies to three-phase and single-phase power transformers (including auto-transformers) with the exception certain categories of small and special transformers such as: -single-phase transformers with rated power less than 1 KV A and three-phase transformers less than 5 KV A; - instrument transformers; - transformers for static convertors; -traction transformers mounted on rolling stock; -starting transformers ; -testing transformers ; -welding transformers ; When standards do not exist for such categories of transformers, this part may still be applicable either as a whole or in part. 1.2 Service conditions This part gives detailed requirement for transformers for use under the following conditions: a)Altitude A height above sea-level not exceeding 1000 m . b) Temperature of ambient air not below - 25℃and not above +40℃.For water-cooled transformers , a temperature of cooling water at the inlet not exceeding +25℃. c) Wave shape of supply voltage A supply voltage of which the wave shape is approximately sinusoidal. NOTE This requirement is normally not critical in public supply systems but may
压力传感器 合理进行压力传感器的误差补偿是其应用的关键。压力传感器主要有偏移量误差、灵敏度误差、线性误差和滞后误差，本文将介绍这四种误差产生的机理和对测试结果的影响，同时将介绍为提高测量精度的压力标定方法以及应用实例。 目前市场上传感器种类丰富多样，这使得设计工程师可以选择系统所需的压力传感器。这些传感器既包括最基本的变换器，也包括更为复杂的带有片上电路的高集成度传感器。由于存在这些差异，设计工程师必须尽可能够补偿压力传感器的测量误差，这是保证传感器满足设计和应用要求的重要步骤。在某些情况下，补偿还能提高传感器在应用中的整体性能。 本文以摩托罗拉公司的压力传感器为例，所涉及的概念适用于各种压力传感器的设计应用。 摩托罗拉公司生产的主流压力传感器是一种单片压阻器件，该器件具有 3 类： 1.基本的或未加补偿标定； 2.有标定并进行温度补偿； 3.有标定、补偿和放大。 偏移量、范围标定以及温度补偿均可以通过薄膜电阻网络实现，这种薄膜电阻网络在封装过程中采用激光修正。 该传感器通常与微控制器结合使用，而微控制器的嵌入软件本身建立了传感器数学模型。微控制器读取了输出电压后，通过模数转换器的变换，该模型可以将电压量转换为压力测量值。传感器最简单的数学模型即为传递函数。该模型可在整个标定过程中进行优化，并且模型的成熟度将随标定点的增加而增加。 从计量学的角度看，测量误差具有相当严格的定义：它表征了测量压力与实际压力之间的差异。而通常无法直接得到实际压力，但可以通过采用适当的压力标准加以估计，计量人员通常采用那些精度比被测设备高出至少 10 倍的仪器作为测量标准。 由于未经标定的系统只能使用典型的灵敏度和偏移值将输出电压转换为压 力，测得的压力将产生如图 1 所示的误差。 这种未经标定的初始误差由以下几个部分组成： a.偏移量误差。由于在整个压力范围内垂直偏移保持恒定，因此变换器扩散和激光调节修正的变化将产生偏移量误差。 b.灵敏度误差，产生误差大小与压力成正比。如果设备的灵敏度高于典型值，灵敏度误差将是压力的递增函数（见图 1）。如果灵敏度低于典型值，那么灵敏度误差将是压力的递减函数。该误差的产生原因在于扩散过程的变化。
毕业设计--基于PLC的变频调速恒压供水系统（含外文翻 译） 山东科技大学学士学位论文摘要 摘要 本论文根据中国城市小区的供水要求，设计了一套基于PLC的变频调速恒压供水系统, 并利用组态软件开发良好的运行管理界面。变频恒压供水系统由可编程控制器、变频器、水泵机组、压力传感器、工控机等构成。 本系统包含三台水泵电机，它们组成变频循环运行方式。采用变频器实现对三相水泵电机的软启动和变频调速，运行切换采用“先启先停”的原则。压力传感器检测当前水压信号，送入PLC与设定值比较后进行PID运算，从而控制变频器的输出电压和频率，进而改变水泵电机的转速来改变供水量，最终保持管网压力稳定在设定值附近。通过工控机与PLC的连接，采用组态软件完成系统监控，实现了运行状态动态显示及数据、报警的查询。 关键词:变频调速，恒压供水，PLC，组态软件 山东科技大学学士学位论文 ABSTRACT ABSTRACT According to the requirement of China's urban water supply, this paper designs a set of water supply system of frequecey control of constant voltage based on PLC, and have developed good operation management interface using Supervision Control and Data Acquisition.The system is made up of PLC, transducer,units of pumps,pressure sensor and control machine and so on.
Circuit breaker 断路器 Compressed air circuit breaker is a mechanical switch equipment, can be i 空气压缩断路器是一种机械开关设备，能够在n normal and special conditions breaking current (such as short circuit cur 正常和特殊情况下开断电流（比如说短路电流）。 rent). For example, air circuit breaker, oil circuit breaker, interference circ 例如空气断路器、油断路器，干扰电路的导体uit conductor for the application of the safety and reliability of the circuit 干扰电路的导体因该安全可靠的应用于其中， breaker, current in arc from is usually divided into the following grades: a 电流断路器按灭弧远离通常被分为如下等级：ir switch circuit breaker, oil circuit breaker, less oil circuit breaker, compr 空气开关断路器、油断路器、少油断路器、压缩空essed air circuit breaker, a degaussing of isolating switch, six sulfur hexaf 气断路器、具有消磁性质的隔离开关、六氟luoride circuit breaker and vacuum breaker. Their parameters of voltage, 化硫断路器和真空断路器。他们的参数有电压等级、current, insulation level of breaking capacity, instantaneous voltage off ti 开断容量的电流、绝缘等级开断时间的瞬时电压恢复和me of recovery and a bombing. Breaker plate usually include: 1 the maxi 轰炸时间。断路器的铭牌通常包括： 1.最大可承
摘要 XF 110KV变电所是地区重要变电所，是电力系统110KV电压等级的重要部分。其设计分为电气一次部分和电气二次部分设计。 一次部分由说明书，计算书与电气工程图组成，说明书和计算书包括变电所总体分析;负荷分析与主变选择;电气主接线设计;短路电流计算;电气设备选择;配电装置选择;变电所总平设计及防雷保护设计。 二次部分由说明书，计算书与电气工程图组成。说明书和计算书包括整体概述;线路保护的整定计算;主变压器的保护整定计算;电容器的保护整定计算;母线保护和所用变保护设计。 计算书和电气工程图为附录部分。其中一次部分电气AutoCAD制图六张；二次部分为四张手工制图。 本变电所设计为毕业设计课题，以巩固大学所学知识。通过本次设计，使我对电气工程及其自动化专业的主干课程有一个较为全面，系统的掌握，增强了理论联系实际的能力，提高了工程意识，锻炼了我独立分析和解决电力工程设计问题的能力，为未来的实际工作奠定了必要的基础。 关键词:变电所；变压器；继电保护
Abstract XF county 110KV substation is an important station in this distract, which is one of the extremely necessary parts of the 110KV network in electric power system. The design of the substation can be separated in two parts: primary part and secondary part of the electric design. The first part consists of specifications, computation book and Electrical engineering drawings about the design. The specifications has several parts which are General analysis of the station, Load analysis, The selection of the main transformer, Layout of configuration, Computation of short circuit; Select of electric devices, Power distribution devices, General design of substation plane and the design of thunderbolt protection. The second part also consists of specifications, computation book and electrical drawings about the design。Specifications and computation book include following section: General, The evaluation and calculate of line protection, Transformer protection, capacitor protection, Bus protection and Self-using transformer protection. Computation book, Electrical engineering drawings and catalogue of drawings are attached in the end。There are nine drawings total, in which four are prepared by hand, others are prepared by computer in which installed the software electrical AutoCAD. From other view, it also can be classified as first part and second part. This is a design of substation for graduation design test. It can strengthen our specified knowledge. Key-words: substation；transformer；Relay protection
Basic knowledge of transducers A transducer is a device which converts the quantity being measured into an optical, mechanical, or-more commonly-electrical signal. The energy-conversion process that takes place is referred to as transduction. Transducers are classified according to the transduction principle involved and the form of the measured. Thus a resistance transducer for measuring displacement is classified as a resistance displacement transducer. Other classification examples are pressure bellows, force diaphragm, pressure flapper-nozzle, and so on. 1、Transducer Elements Although there are exception ,most transducers consist of a sensing element and a conversion or control element. For example, diaphragms,bellows,strain tubes and rings, bourdon tubes, and cantilevers are sensing elements which respond to changes in pressure or force and convert these physical quantities into a displacement. This displacement may then be used to change an electrical parameter such as voltage, resistance, capacitance, or inductance. Such combination of mechanical and electrical elements form electromechanical transducing devices or transducers. Similar combination can be made for other energy input such as thermal. Photo, magnetic and chemical,giving thermoelectric, photoelectric,electromaanetic, and electrochemical transducers respectively. 2、Transducer Sensitivity The relationship between the measured and the transducer output signal is usually obtained by calibration tests and is referred to as the transducer sensitivity K1= output-signal increment / measured increment . In practice, the transducer sensitivity is usually known, and, by measuring the output signal, the input quantity is determined from input= output-signal increment / K1. 3、Characteristics of an Ideal Transducer The high transducer should exhibit the following characteristics a) high fidelity-the transducer output waveform shape be a faithful reproduction of the measured; there should be minimum distortion. b) There should be minimum interference with the quantity being measured; the presence of the transducer should not alter the measured in any way. c) Size. The transducer must be capable of being placed exactly where it is needed.
2020年外文翻译模板 精编版
精品好文档，推荐学习交流 华北电力大学 毕业设计（论文）附件 外文文献翻译 学号：201001000826姓名：郑蓓 所在院系：电力工程系专业班级：电力1002 指导教师：刘英培 原文标题：Simulation of PMSM Vector Control System based on Non-linear PID and Its Easy DSP Realization 2014年4月10日
基于非线性PID永磁同步电机矢量控制系统仿真及其DSP实现 摘要 本文给出空间矢量脉宽调制（SVPWM）的基本原理，以及构建两条闭合回路矢量控制永磁同步电机（PMSM）的仿真模型方法。同时，在速度闭环对于新型非线性PID控制器进行了研究。仿真结果表明它具有无超调和小速度脉动良好的动态和静态性能。此外，利用在MATLAB中嵌入式目标为TI C2000（C2000 ETTI）的工具，我们将SVPWM仿真模型转换成可执行代码，并下载到TMS320F2812，实现基于DSP永磁同步电机的开环控制。这种方法避免了繁琐的编程工作，缩短了系统开发周期，实现了同步模拟和DSP实现永磁同步电机矢量控制系统的目标。 1 引言 永磁同步电机被广泛使用在交流伺服系统，因为它有如快速响应，出色的操控性能，尺寸小和重量轻等优点。最近，SVPWM技术逐渐取代了传统的SPWM。SVPWM的目的是产生磁通矢量来接近交流电机实际气隙磁通圆，通过在逆变器装置调整切换时间和控制电功率的通断模式。相较于SPWM，SVPWM 技术降低了谐波含量和开关损耗，其直流电压利用率也提高了很多。此外，它很容易被数字化。因此，我们在本文应用SVPWM技术。 原文出处及作者：Wang Song; Shi Shuang-shuang; Chen Chao, "Simulation of PMSM vector control system based on non-linear PID and its easy DSP realization," Control and Decision Conference, 2009. CCDC '09. Chinese , vol., no., pp.949,953, 17-19 June 2009
Sensor technology A sensor is a device which produces a signal in response to its detecting or measuring a property ,such as position , force , torque , pressure , temperature , humidity , speed , acceleration , or vibration .Traditionally ,sensors (such as actuators and switches )have been used to set limits on the performance of machines .Common examples are (a) stops on machine tools to restrict work table movements ,(b) pressure and temperature gages with automatics shut-off features , and (c) governors on engines to prevent excessive speed of operation . Sensor technology has become an important aspect of manufacturing processes and systems .It is essential for proper data acquisition and for the monitoring , communication , and computer control of machines and systems . Because they convert one quantity to another , sensors often are referred to as transducers .Analog sensors produce a signal , such as voltage ,which is proportional to the measured quantity .Digital sensors have numeric or digital outputs that can be transferred to computers directly .Analog-to-coverter(ADC) is available for interfacing analog sensors with computers . Classifications of Sensors Sensors that are of interest in manufacturing may be classified generally as follows: Machanical sensors measure such as quantities as positions ,shape ,velocity ,force ,torque , pressure , vibration , strain , and mass . Electrical sensors measure voltage , current , charge , and conductivity . Magnetic sensors measure magnetic field ,flux , and permeablity . Thermal sensors measure temperature , flux ,conductivity , and special heat . Other types are acoustic , ultrasonic , chemical , optical , radiation , laser ,and fiber-optic . Depending on its application , a sensor may consist of metallic , nonmetallic , organic , or inorganic materials , as well as fluids ,gases ,plasmas , or semiconductors .Using the special characteristics of these materials , sensors covert the quantity or property measured to analog or digital output. The operation of an ordinary mercury thermometer , for example , is based on the difference between the thermal expansion of mercury and that of glass. Similarly , a machine part , a physical obstruction , or barrier in a space can be detected by breaking the beam of light when sensed by a photoelectric cell . A proximity sensor ( which senses and measures the distance between it and an object or a moving member of a machine ) can be based on acoustics , magnetism , capacitance , or optics . Other actuators contact the object and take appropriate action ( usually by electromechanical means ) . Sensors are essential to the conduct of intelligent robots , and are being developed with capabilities that resemble those of humans ( smart sensors , see the following ). This is America, the development of such a surgery Lin Bai an example, through the screen, through a remote control operator to control another manipulator, through the realization of the right abdominal surgery A few years ago our country the