y = ym sin(3.38 + 261t + 0.129 x)
y = A sin( phi0 + w t + k x )
(A) wavelength = 2 pi / k = 2 pi / 0.129 = 48.7 m
(B) f = w / 2pi = 261 / 2pi = 41.5 Hz
(C) T = 1/f = 0.024 s
(D) phi0 = 3.38 rad
A general traveling wave can be expressed as
where is the wavenumber, is the angular frequency, and is called the phase constant. Alternatively, a cosine function could be used in the place of the sine function (which would alter the value of , and nothing else). The order of the three terms is unimportant, but is always the coefficient of the position () and is always the coefficient of the time (). Therefore, the wavenumber, angular frequency, and phase constant are
The wavelength is related to , whereas the temporal properties (frequency and period) are related to . To see how, start with the fact that sine (or cosine) repeats every radians. The phase constant does not change, so at a fixed time, the distance over which the waveform repeats is called the wavelength. So, putting the wavelength () in place of the distance (), the product of the wavenumber and the wavelength must be equal to radians.
Conversely, at a fixed position, the time over which the waveform repeats is called the period. Putting the period () in place of the time (), the product of the angular frequency and the period must be equal to radians.
The frequency () is just the inverse of the period, and it expresses how many oscillations a fixed position goes through per unit time.
Consider the waveform expression. y(x, t) = Ymsin (3.38 + 261t + 0.129x) The transverse displacement...
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y(x,t)=
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y(x, t) = A cos(kx − ωt − φ)
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Please show clear steps of how
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(1 point) The graph shows the displacement from equilibrium of a mass-spring system as a function of time after the vertically hanging system was set in motion at time t 0. Assume that the units of time are seconds, and the units of displacement are centimeters. The first t-intercept is (0.75, 0) and the first minimum has coordinates (1.25, -4). (a) What is the period T of the periodic motion? seconds...
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