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Simple Nature - Light and Matter

Simple Nature - Light and Matter

Simple Nature - Light and Matter

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itself, <strong>and</strong> since the body is very massive, the behavior of the waveswhen they reach the end of the string can be understood in thesame way as if the actual guitar string was attached on the ends tostrings that were extremely massive. Reflections are most intensewhen the two media are very dissimilar. Because the wave speed inthe body is so radically different from the speed in the string, weshould expect nearly 100% reflection.Although this may seem like a rather bizarre physical model ofthe actual guitar string, it already tells us something interestingabout the behavior of a guitar that we would not otherwise haveunderstood. The body, far from being a passive frame for attachingthe strings to, is actually the exit path for the wave energy in thestrings. With every reflection, the wave pattern on the string losesa tiny fraction of its energy, which is then conducted through thebody <strong>and</strong> out into the air. (The string has too little cross-section tomake sound waves efficiently by itself.) By changing the propertiesof the body, moreover, we should expect to have an effect on themanner in which sound escapes from the instrument. This is clearlydemonstrated by the electric guitar, which has an extremely massive,solid wooden body. Here the dissimilarity between the two wavemedia is even more pronounced, with the result that wave energyleaks out of the string even more slowly. This is why an electricguitar with no electric pickup can hardly be heard at all, <strong>and</strong> it isalso the reason why notes on an electric guitar can be sustained forlonger than notes on an acoustic guitar.If we initially create a disturbance on a guitar string, how willthe reflections behave? In reality, the finger or pick will give thestring a triangular shape before letting it go, <strong>and</strong> we may think ofthis triangular shape as a very broad “dent” in the string whichwill spread out in both directions. For simplicity, however, let’s justimagine a wave pattern that initially consists of a single, narrowpulse traveling up the neck, m/1. After reflection from the top end,it is inverted, m/3. Now something interesting happens: figure m/5is identical to figure m/1. After two reflections, the pulse has beeninverted twice <strong>and</strong> has changed direction twice. It is now back whereit started. The motion is periodic. This is why a guitar producessounds that have a definite sensation of pitch.self-check FNotice that from m/1 to m/5, the pulse has passed by every point on thestring exactly twice. This means that the total distance it has traveledequals 2 L, where L is the length of the string. Given this fact, what arethe period <strong>and</strong> frequency of the sound it produces, expressed in termsof L <strong>and</strong> v, the velocity of the wave? ⊲ Answer, p. 924Note that if the waves on the string obey the principle of superposition,then the velocity must be independent of amplitude, <strong>and</strong>the guitar will produce the same pitch regardless of whether it iso / The period of this doublepulsepattern is half of what we’dotherwise expect.p / Any wave can be madeby superposing sine waves.Section 6.2 Bounded Waves 371

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