ENVS 1200 Chapter Notes - Chapter 7: Carrier Wave, Musical Tone, Hertz

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ENVS 1200 Chapter 7 Notes Summary
Introduction
Materials that are not transparent can be used to guide or reflect a wave.
A satellite dish, for example, works by reflecting radio waves from the dish to a single
point, where they are concentrated and collected by a sensitive receiver.
Similarly, fiber-optic cables maximize the light at the receiving end of the cable by
guiding the light through the cable.
In practice, the sine waves that we have discussed are of limited use by themselves.
A sound made up of a sine wave produces a single, pure tone.
A 440-Hz sie ae produces the toe called A, for exaple.
There is not much useful information value (or musical interest) in a pure sine wave
tone.
Instead, sine waves are used as carriers for the data that we wish to transmit.
We modulate, or change, one or more of the three characteristics of the sine wave,
amplitude, frequency, or phase, to represent the signal that is to be transmitted.
Thus, an AM, or amplitude-modulated, radio station at 1100 KHz would use a sine wave
carrier of 1100 KHz.
The music broadcast on that station would modulate the amplitude of the carrier to
correspond to the sound of the music.
The AM station uses only one type of modulation.
You should be able to guess what kind of modulation is used by an FM station!
To restore the original waveform that was used to modulate the carrier, we use a
demodulator or detector.
An example of carrier amplitude modulated by another analog signal is shown
Note that amplitude modulation is symmetric with respect to the center of the carrier
sine wave.
For digital signals, the carrier signal is modulated with only two possible values, the
alue represetig a  ad the alue represetig a .
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