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mechanical vibrations explained

standing waves continuous systems

Let the masses go to infinity and you get a string or beam; the modes are integer-multiple standing waves fₙ = n·f₁ (harmonics), pitch set by f₁ = (1/2L)√(T/μ)

In the last lesson, N masses meant N modes. Stretch those masses without end until they become one continuous string, and the modes become endless too. Each mode is a smooth standing wave with both ends held fixed, and its frequency is a whole-number multiple of the fundamental. That is why a string becomes music. The moment the masses crowd into a curve, vibration starts to speak the language of waves.

Raise N. With only a few masses the mode shape is still the jagged one from the last lesson, but as the count grows it gathers into one smooth curve, a continuous string. A continuous system is a multi-degree system whose masses never run out. When the gaps between the points disappear, the shape is read as a curve.

The simplest mode is the fundamental. The whole string rises and falls as one arch, with both ends held as nodes. Half a wavelength equals the length of the string, so λ₁ = 2L, and the frequency is the lowest one, f₁. The middle moves the most, and the ends do not move.

Choose a higher mode. The nth mode has n arches, and between them there are n−1 nodes. The frequency is fₙ = n·f₁, a whole-number multiple of the fundamental. That ladder of whole multiples is the harmonic series, and it is why a string sounds musical. The more nodes there are, the higher the pitch.

The superposition of A5 spreads across endless modes. Pluck the string at one point and that triangle is a sum of standing-wave modes. Add more harmonics and the corner grows sharp, gathering toward the plucked shape. Which mix you chose is the tone color. Fewer harmonics leave a round corner, and more of them make the plucked point distinct.

What sets the pitch? f₁ = (12L)√(Tμ), so the tension T, the length L, and the linear density μ decide it. Move the three. Tighter (T↑), shorter (L↓, which is fretting), or thinner (μ↓) raises the pitch. A bass string is thick for the same reason, and bridge cables and power lines hum by the same formula. Tighter, shorter, and lighter means a higher pitch.

In PracticeA continuous system, a string or a beam or a plate, is a multi-degree system whose masses never run out, so its modes never run out either. Each mode is a standing wave between nodes at the two ends, and on a string the frequency is fₙ = n·f₁, a whole-number multiple of the fundamental, a harmonic. Any vibration splits into a sum of these modes, and plucked shape = sum of harmonics = tone color. The fundamental is f₁ = (12L)√(Tμ), set by tension, length, and linear density. Practice is always the same. Find the shape and the frequency of each mode, and keep the drive off all of them. A bridge, a wing, and a building are continuous bodies with endless modes too, and the standing wave is where vibration meets waves and music. That meeting is the point of this lesson.
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