#$&* course phy 202 If your solution to stated problem does not match the given solution, you should self-critique per instructions at
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Given Solution: ** we know how many wavelength segments will pass every second, and we know the length of each, so that multiplying the two gives us the velocity with which they must be passing ** Your Self-Critique: ok Your Self-Critique Rating: ok ********************************************* Question: explain how we can reason out that the period of a periodic wave is equal to its wavelength divided by its velocity YYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYY Your Solution: Well, I have previously shown that the velocity of the wave is equal to the frequency times the wavelength. The period of the wave is equal to the inverse of the frequency (T = 1/f or f = 1/T). If I substitute this relationship into the formula that I already know and rearrange it, then I can show that the period is equal to the wavelength divided by velocity: v = f*’lambda v = (1/T)*lambda T*v = lambda T = lambda/v confidence rating #$&*: ^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^
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Given Solution: ** If we know how far it is between peaks (wavelength) and how fast the wavetrain is passing (velocity) we can divide the distance between peaks by the velocity to see how much time passes between peaks at a given point. That is, period is wavelength / velocity. ** Your Self-Critique: ok Your Self-Critique Rating: ok ********************************************* Question: explain why the equation of motion at a position x along a sinusoidal wave is A sin( `omega (t - x / v) ) if the equation of motion at the x = 0 position is A sin(`omega t) YYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYY Your Solution: If the equation of motion at x=0 is A*sin(‘omega t), then there is a point at an arbitrary distance x that also follows this motion. This position x occurs at a “time lag”. The time lag is equal to x/v. Therefore, the equation for the y position at the arbitrary point x is now: y = A sin(‘omega (t - “time lag”)) y = A sin(‘omega (t - x/v)) confidence rating #$&*: ^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^
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Given Solution: ** the key is the time delay. Time for the disturbance to get from x = 0 to position x is x / v. What happens at the new position is delayed by time x/v, so what happens there at clock time t happened at x=0 when clock time was t = x/v. In more detail: If x is the distance down the wave then x / v is the time it takes the wave to travel that distance. What happens at time t at position x is what happened at time t - x/v at position x=0. That expression should be y = sin(`omega * (t - x / v)). The sine function goes from -1 to 0 to 1 to 0 to -1 to 0 to 1 to 0 ..., one cycle after another. In harmonic waves the motion of a point on the wave (think of the motion of a black mark on a white rope with vertical pulses traveling down the rope) will go thru this sort of motion (down, middle, up, middle, down, etc.) as repeated pulses pass. If I'm creating the pulses at my end, and that black mark is some distance x down in rope, then what you see at the black mark is what I did at time x/v earlier. ** STUDENT COMMENT (University Physics): According to the Y&F book (p.553) we get the expression for a sinusoidal wave moving the the +x-direction with the equation: Y(x,t) = A*cos[omega*(t-x/v)] I am not sure where the sine came from in the equation in the question. The book uses the cosine function to represent the waves motion.