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== Boundary conditions == Where the nodes occur in relation to the boundary reflecting the waves depends on the end conditions or [[boundary conditions]]. Although there are many types of end conditions, the ends of resonators are usually one of two types that cause total reflection: *<u>Fixed boundary</u>: Examples of this type of boundary are the attachment point of a [[guitar]] string, the closed end of an open pipe like an [[organ pipe]], or a [[woodwind]] pipe, the periphery of a [[drumhead]], a [[transmission line]] with the end [[short circuit]]ed, or the mirrors at the ends of a [[laser cavity]]. In this type, the amplitude of the wave is forced to zero at the boundary, so there is a node at the boundary, and the other nodes occur at multiples of half a wavelength from it:{{block indent | text = 0, 位/2, 位, 3位/2, 2位, ..., n位/2}} *<u>Free boundary</u>: Examples of this type are an open-ended organ or woodwind pipe, the ends of the vibrating resonator bars in a [[xylophone]], [[glockenspiel]] or [[tuning fork]], the ends of an [[Antenna (radio)|antenna]], or a transmission line with an open end. In this type the [[derivative (calculus)|derivative]] (slope) of the wave's amplitude (in [[sound wave]]s the pressure, in electromagnetic waves, the [[Electric current|current]]) is forced to zero at the boundary. So there is an amplitude maximum (antinode) at the boundary, the first node occurs a quarter wavelength from the end, and the other nodes are at half wavelength intervals from there: {{block indent | text = 位/4, 3位/4, 5位/4, 7位/4, ..., (2n+1)位/4}}
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