英文翻译外文文献翻译23毕业设计外文英文翻译射频与微波应用.doc
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1、附录A 英文原文Radio Frequency and Microwave ApplicationsA.1 IntroductionThis chapter lays the foundation for understanding higher-frequency wave phenomena and divides the task of active circuit design for RE/MV frequencies into specific concept blocks. These concept blocks create a gradual approach to und
2、erstanding and designing RF/MW circuits and represent specific realms of knowledge that need to be mastered to become an accomplished designer.Before we describe and analyze these types of waves we need to consider why RF/microwaves as a subject has become so important, that it is placed at the fore
3、front of our modern technology. Furthermore, we need to expand our minds to the many possibilities that these signals can provide for peaceful practices by exploring various commercial applications useful to mankind.A 1.1 A Short History of RF and MicrowavesCirca 18641873, James Clark Maxwell integr
4、ated the entirety of mans knowledge of electricity and magnetism by introducing a set of four coherent and self-consistent equations that describe the behavior of electric and magnetic fields on a classical level. This wav the beginning of microwave engineering, as presented in a treatise by Maxwell
5、 at that time .He predicted, purely from a mathematical standpoint and on a theoretical basis, the existence of electromagnetic wave propagation and that light was also a from of electromagnetic energy both completely new concepts at the time.From 1885 to 1887, Oliver Heaviside simplified Maxwells w
6、ork in his published papers. From 1887 to 1891, a German physics professor, Heinrich Hertz, verified Maxwells predictions experimentally and demonstrated the propagation of electromagnetic wave. He also investigated wave propagation phenomena along transmission line and antennas and developed severa
7、l useful structures. He could be called the first microwave engineer.Marconi tried to commercialize radio at a much lower frequency for long-distance communications, but as he had a business interest in all of his work and developments, this was not a purely scientific endeavor.Neither Hertz nor Hea
8、viside investigated the possibility of electromagnetic wave propagation inside a hollow metal tube because it was felt that two conductors were necessary for the transfer of electromagnetic wave or energy. In 1897, Lord Rayleigh showed mathematically that electromagnetic wave propagation was possibl
9、e in wave-guides, both circular and rectangular. He showed that there are infinite sets of modes of the TE and TM type possible, each with its own cut-off frequency. These were all theoretical predictions with no experimental verifications.From 1897 to 1936, the wave-guide was essentially forgotten
10、until two men, George Southworth (AT&T) and W. L. Barron (MIT), who showed experimentally that a wave-guide could be used as small bandwidth transmission medium, capable of carrying high power signals.With the invention of the transistor in the 1950s and the advent of microwave integrated circuits i
11、n the 1960s, the concept of a microwave system on a chip became a reality. There have been many other developments, mostly in terms of application mass, that have made RF and microwave an enormously useful and popular subject. Maxwells equations laid the foundation and laws of the science of electro
12、magnetic, of which the field of RF and microwave is a small subset. Due to the exact and all-encompassing nature of these laws in predicting electromagnetic phenomena, along with the great body of analytical and experimental investigations performed since then, we can consider the field of RF and mi
13、crowave engineering a “mature discipline” at this time.A.1.2 Applications of Maxwells Equations As indicated earlier in Chapter 2, Fundamental Concepts in Electrical and Electronics Engineering, standard circuit theory can neither be use at RF nor particularly at microwave frequencies. This is becau
14、se the dimensions of the device or components are comparable to the wavelength, which means that phase of an electrical signal (e.g., a current or voltage) changes significantly over the physical length of the device or component. Thus use of Maxwells equations at these higher frequencies becomes im
15、perative. In contrast, the signal wavelengths at lower frequencies are so much larger than the device or component dimensions, that these are negligible variation in phase across the dimensions of the circuit. Thus Maxwells equations simplify into basic circuit theory, as covered in Chapter 3, Mathe
16、matical Foundation for Understanding Circuits. At the other extreme of the frequency range lies the optical field, where the wavelength is much smaller than the device or circuit dimensions. In this case, Maxwells equations simplify into a subject commonly referred to as geometrical optics, which tr
17、eats light as a ray traveling on a straight line. These optical techniques may be applied successfully to the analysis of very high microwave frequencies (e.g., high millimeter wave range),where they are referred to as “quasi-optical.” Of course, it should be noted that further application of Maxwel
18、ls equation leads to an advanced field of optics called “physical apices or Fourier optics,” which treats light as a wave and explains such phenomena as diffraction and interference, where geometrical optics fails completely. The important conclusion to be drawn from this discussion is that Maxwells
19、 equations present a unified theory of analysis for any system at any frequency, provided we use appropriate simplifications when the wavelengths involved are much larger, comparable to, or much smaller than the circuit dimensions.A.1.2 Properties of RF and Microwaves An important property of signal
20、s at RF, and particularly at higher microwave frequencies, is their great capacity to carry information. This is due to the large bandwidths available at these high frequencies. For example, a 10 percent bandwidth at 60MHz carrier signal is 6MHz, which is approximately one TV channel of information;
21、 on the other hand 10 percent of a microwave carrier signals at 60 GHz is 6GHz, which is equivalent to 1000 TV channels. Another property of microwaves is that they travel by line of sight, very much like the traveling of light rays, as described in the field of geometrical optics. Furthermore, unli
22、ke lower-frequency signals, microwave signals are not bent by ionosphere. Thus use of line-of-sight communication towers or links on the ground and orbiting satellites around the globe are a necessity for local or global communications. A very important civilian as well as military instrument is rad
23、ar. The concept of radar is based on radar cross-section which is the effective reflection area of the target. A targets visibility greatly depends on the targets electrical size, which is a function of the incident signals wavelength. Microwave frequency is the ideal signal band for radar applicati
24、ons. Of course, another important advantage of use of microwaves in radars is the availability of higher antenna gain as the frequency is increased for a given physical antenna size. This is because the antenna gain being proportional to the electrical size of the antenna becomes larger as frequency
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