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The next layer encompasses [link] through [link] . This gives a closer look at the idealized receiver—how things work when everythingis just right: when the timing is known, when the clocks run at exactly the right speed, when there are no reflections,diffractions, or diffusions of the electromagnetic waves. This layer also introduces a few M atlab tools that are needed to implement the digital radio.The order in which topics are discussed is precisely the order in which they appear in the receiver:

channel C h a p t e r 4 frequency translation C h a p t e r 5 sampling C h a p t e r 6
receive filtering equalization C h a p t e r 7 decision device decoding C h a p t e r 8
Channel impairments and linear systems Chapter 4 Frequency translation and modulation Chapter 5 Sampling and gain control Chapter 6 Receive (digital) filtering Chapter 7 Symbols to bits to signals Chapter 8

Chapter  [link] provides a complete (though idealized) software-defined digital radio system.

From there to here, from here to there, funny things are everywhere.

—Dr. Seuss, One Fish, Two Fish, Red Fish, Blue Fish, 1960

If every signal that went from here to there arrived at its intended receiver unchanged, the life of a communications engineerwould be easy. Unfortunately, the path between here and there can be degraded in several ways, including multipath interference,changing (fading) channel gains, interference from other users, broadband noise, and narrowband interference.

This chapter begins by describing these problems, which are diagrammed in [link] . More important than locating the sources of the problems isfixing them. The received signal can be processed using linear filters to help reduce the interferencesand to undo, to some extent, the effects of the degradations. The central question is how to specify filters that can successfullymitigate these problems, and answering this requires a fairly detailed understanding of filtering.Thus, a discussion of linear filters occupies the bulk of this chapter, which also provides a background for other uses of filtersthroughout the receiver, such as the lowpass filters used in the demodulators of Chapter  [link] , the pulse shaping and matched filters of Chapter  [link] , and the equalizing filters of Chapter  [link] .

When bad things happen to good signals

The path from the transmitter to the receiver is not simple, as [link] suggests. Before the signal reaches the receiver, it is subjectto a series of possible “funny things,” events that may corrupt the signal and degrade the functioning of the receiver.This section discusses five kinds of corruption that are used throughout the chapter to motivate and explain the various purposesthat linear filters may serve in the receiver.

Other users

Many different users must be able to broadcast at the same time. This requires that there be a way for areceiver to separate the desired transmission from all the others (for instance, to tune to a particular radio or TV station among a largenumber that may be broadcasting simultaneously in the same geographical region). One standard method is to allocate different frequencybands to each user. This was called frequency division multiplexing (FDM) in Chapter  [link] , and was shown diagrammatically in [link] . The signals from the different users can be separatedusing a bandpass filter, as in [link] . Of course, practical filters do not completely remove out-of-bandsignals, nor do they pass in-band signals completely without distortions. Recall the three filters in [link] .

Questions & Answers

A golfer on a fairway is 70 m away from the green, which sits below the level of the fairway by 20 m. If the golfer hits the ball at an angle of 40° with an initial speed of 20 m/s, how close to the green does she come?
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cm
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A mouse of mass 200 g falls 100 m down a vertical mine shaft and lands at the bottom with a speed of 8.0 m/s. During its fall, how much work is done on the mouse by air resistance
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Can you compute that for me. Ty
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Chemistry is a branch of science that deals with the study of matter,it composition,it structure and the changes it undergoes
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2. A sled plus passenger with total mass 50 kg is pulled 20 m across the snow (0.20) at constant velocity by a force directed 25° above the horizontal. Calculate (a) the work of the applied force, (b) the work of friction, and (c) the total work.
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you have been hired as an espert witness in a court case involving an automobile accident. the accident involved car A of mass 1500kg which crashed into stationary car B of mass 1100kg. the driver of car A applied his brakes 15 m before he skidded and crashed into car B. after the collision, car A s
Samuel Reply
can someone explain to me, an ignorant high school student, why the trend of the graph doesn't follow the fact that the higher frequency a sound wave is, the more power it is, hence, making me think the phons output would follow this general trend?
Joseph Reply
Nevermind i just realied that the graph is the phons output for a person with normal hearing and not just the phons output of the sound waves power, I should read the entire thing next time
Joseph
Follow up question, does anyone know where I can find a graph that accuretly depicts the actual relative "power" output of sound over its frequency instead of just humans hearing
Joseph
"Generation of electrical energy from sound energy | IEEE Conference Publication | IEEE Xplore" ***ieeexplore.ieee.org/document/7150687?reload=true
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progressive wave
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Mujahid
A string is 3.00 m long with a mass of 5.00 g. The string is held taut with a tension of 500.00 N applied to the string. A pulse is sent down the string. How long does it take the pulse to travel the 3.00 m of the string?
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Source:  OpenStax, Software receiver design. OpenStax CNX. Aug 13, 2013 Download for free at http://cnx.org/content/col11510/1.3
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