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Free , online service which translates office documents ( Word , Excel, Powerpoint, PDF , OpenOffice, text) into multiple languages, preserving the original layout. laws is beyond the scope of this book, they deserve to be mentioned here at least briefly James Clerk Maxwell was the first to correctly assemble the complete laws of electrodynamics in this classic text Modern electromagnetism theory is based on the four fundamental equations known as Maxwell s equations Before Maxwell, the laws of electrodynamics, including Gauss s Law, Ampere s Law of Magnetostatics, and Faraday s Law, were laws of electrostatics and did not predict waves These laws correctly described what is known as the near field (that is, the electrostatic field of an electric charge and the magnetostatic field of a current loop) These laws described the observable impact of electric charges and magnetic fields close to the source but failed to describe the distant impact of these forces In the static case, when all electric charges are permanently fixed or if they all move at a steady state, the electric field and the magnetic field are not interconnected This allows us to study electricity and magnetism as two distinct and separate phenomena Up until Maxwell challenged conventional wisdom, the separation of electricity and magnetism was the accepted state of the world He corrected Ampere s Law of Magnetostatics to become Ampere s Law, so that consistency with the Law of Conservation of Charge occurred Maxwell added a term indicating that vortices of magnetic fields can be displacement current density (time-varying electric flux density) as well as conduction current density The resulting corrected equations define the complete laws of electrodynamics and predict electromagnetic waves Heinrich Rudolf Hertz confirmed experimentally that these waves exist Maxwell showed that any conductor (eg, antenna) supplied with an alternating current produces a varying magnetic field (H-field), which in turn produces electric field lines (E-field) in space This is termed the near field In the near field both the E- and H-fields are relatively static with no propagation They only vary in strength as the current varies, with the magnetic flux of the H-field coming out from the antenna and going back in, and the E-field emanating outward Maxwell also proved that beyond this quasi-static near field, both the E-fields and H-fields at a certain distance detached themselves from the conductor and propagated into free space as a combined wave, moving at the speed of light with a constant ratio of E/H = 120 or 377 The point in which this happens is called the far field Maxwell s equations beautifully and correctly describe both the energy storage field and the energy propagation field It was the physicist Ludwig Boltzmann who said, There is nothing more practical than a good theory, and that is absolutely true in the case of Maxwell s equations; although highly theoretical and mathematical in their nature, they provided an unprecedented contribution to our. free pdf to word converter online which is editable: PDF to DOC – Convert PDF to Word Online best pdf to word converter online Free Online OCR - Convert JPEG, PNG, GIF, BMP, TIFF, PDF , DjVu ...
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Do you want to convert an PDF file to Word ? Don't download software - use Zamzar to convert it for free online . Click to convert your PDF file now. and 19 dB, respectively The result is that these modulation methods, from the microwave link design prospective with a high number of states, are very inefficient in dense city networks containing many randomly oriented links (eg, a mesh network) If the size of antennas in both ends is doubled, roughly 6 + 6 dB can be gained Due to practical reasons, antenna gains exceeding about 44 dB cannot be used With these changes, 12 15 dB is possible and, in the case of short hops, the missing part may be covered by the excess system gain margin If the RF channel can be changed from 28 56 MHz, this kind of capacity upgrade will be less critical, because 32TCM can be used The system gain increase demand would then be only 4 dB and could be partly covered by transmit power increase (eg, 3 dB) or with a 50 percent bigger antenna at one end If antenna changes are planned, the rigidity and available space of the supporting structures must be checked If antenna changes are not possible, the hop lengths normally must be reduced The general rule is that, to obtain higher data rates, higher-order modulation schemes must be employed Sophisticated modulation methods for high SDH capacity links can improve the spectral efficiency, but the price paid for this increased throughput is an increase in operating threshold level (and more susceptibility to interference) In real terms, the trade-off is data rate versus energy per bit, and thus range Since an increase in bandwidth normally introduces an increase in error rate, error-correcting schemes (overhead) are often included to produce a net gain in data throughput Detailed information on the subject of spectrum efficiency is provided in ITU-R Recommendation SM1046 6237 Coded Modulation This is a technique that combines coding and modulation that would have been done independently in the conventional method Redundant bits are inserted in multistate numbers of transmitted signal constellations This process is known as coded modulation Representative examples of coded modulation are block coded modulation (BCM), trellis coded modulation (TCM), and multilevel coded modulation (MLC or MLCM) In BCM, levels are coded by block codes, whereas TCM uses only convolutional codes TCM uses the same modulation scheme as QAM, but it adds an extra bit to every symbol for error control purposes On the other hand, different codes can be used for each coded level in MLCM, so MLCM can be seen as a general concept that includes BCM and, to some extent, TCM These schemes require added receiver complexity in the form of a maximum likelihood decoder with soft decision convert pdf to word with marathi font online Convert PDF to Word - SimplyPDF
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