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Unformatted text preview: Generic equation for a wave traveling in positive xdirection with wave speed v : ) ( ) , ( vt x f t x y − = Therefore the disturbance is the same, as long as is constant, say x vt x x vt x + = ⇒ = − A point of constant disturbance, y ( x ) , (crest, trough, etc.) moves at the wave speed, v Here can be ANY function. The type of the function specifies the shape of the wave. ) ( x f ) ( x f How do we know it is a propagating (traveling) wave? (the disturbance) depends on and in a VERY SPECIAL WAY: it only depends on y x t vt x − y vt x − x vt x = − ) , ( ) , ( x y t x y = Example: a bellshaped (Gaussian) curve with a peak at = x ) exp( ) ( ) ( 2 x x f x y − = = A bellshaped (Gaussian) curve with a peak at b x = ] ) ( exp[ ) ( 2 b x x y − − = What if the peak is moving along the x axis with a speed ? v We can plug in and get vt b = ] ) ( exp[ ) ( ) , ( 2 vt x vt x f t x y − − = − = The answer we arrived at: ] ) ( exp[ ) ( ) , ( 2 vt x vt x f t x y − − = − = How do we understand it? y(x,t) is the value of the disturbance at the point and time of interest, x , and t How does the profile of the disturbance y(x,t) look at time t 1 ? It is ] ) ( exp[ ) , ( 2 1 1 vt x t x y − − = a Gaussian function with maximum at 1 vt x = vt x = As usual for a wave, the position of the maximum is given by vt x = max The position of the maximum, the crest, moves at the wave speed, v Wave on a string Any way to calculate the wave speed? What is it likely to depend on?...
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This note was uploaded on 12/13/2011 for the course PHYS 2C PHYS 2C taught by Professor Groisman during the Spring '11 term at UCSD.
 Spring '11
 groisman

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