12) The figure below shows the maximum displacement for a standing wave patter. The earliest time between the two flashes (the solid and the dotted lines] is 0.025 s. The wave functions for the two waves that interfere to produce the standing wave pattern shown in the figure are: 1%3D0

College Physics
11th Edition
ISBN:9781305952300
Author:Raymond A. Serway, Chris Vuille
Publisher:Raymond A. Serway, Chris Vuille
Chapter1: Units, Trigonometry. And Vectors
Section: Chapter Questions
Problem 1CQ: Estimate the order of magnitude of the length, in meters, of each of the following; (a) a mouse, (b)...
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4 mm --
1=0.025 s
0.5 m →
(a) y(x, t) = 2mm sin(2nx)cos(20nt)
(b)y(x, t) = 4mm sin(2nx)cos(20xt)
(C) y(x, t) = 2mm sin(4rx)cos(20xt)
(d)y(x, t)
- 2mm sin(2x)cos(40nt)
12) The figure below shows the maximum displacement for a standing wave pattern. The earliest time
between the two flashes (the solid and the dotted lines) is 0.025 s. The wave functions for the two
waves that interfere to produce the standing wave pattern shown in the figure are:
1=0.025 s
-05 m
(a) y,(x,t) = 2mm sin(4nx 20nt) and y,6x,t) 2mm sin(4nx +20nt)
(b) y,(x, t) = 2mm sin(2nx - 40nt) and y,(x, t)
(c) y (x, t) = 1mm sin(2nx 20nt) and y, (x,t) 1mm sin(2nx + 20nt)
(d) y, (x, t) = 1mm sin(2nx – 40nt) and y,(x, t)= 1mm sin(2rx + 40rt)
= 2mm sin(2mx+40xt)
%3D
%3D
13) A bucket full of water hangs from one end of a string that passes over a light pulley. The other end of
the string is driven by an oscillator of constant frequency, and the fundamental mode of standing waves
is observed with one loop formed between the oscillatorand the pulley Holes are poked in the bucket
causing it to start leaking water. When the bucket's mass drops to 1/4 of its initial value,
oscillator
pulley
oscillator
pulley
kaking
bucket
water-filled
Transcribed Image Text:4 mm -- 1=0.025 s 0.5 m → (a) y(x, t) = 2mm sin(2nx)cos(20nt) (b)y(x, t) = 4mm sin(2nx)cos(20xt) (C) y(x, t) = 2mm sin(4rx)cos(20xt) (d)y(x, t) - 2mm sin(2x)cos(40nt) 12) The figure below shows the maximum displacement for a standing wave pattern. The earliest time between the two flashes (the solid and the dotted lines) is 0.025 s. The wave functions for the two waves that interfere to produce the standing wave pattern shown in the figure are: 1=0.025 s -05 m (a) y,(x,t) = 2mm sin(4nx 20nt) and y,6x,t) 2mm sin(4nx +20nt) (b) y,(x, t) = 2mm sin(2nx - 40nt) and y,(x, t) (c) y (x, t) = 1mm sin(2nx 20nt) and y, (x,t) 1mm sin(2nx + 20nt) (d) y, (x, t) = 1mm sin(2nx – 40nt) and y,(x, t)= 1mm sin(2rx + 40rt) = 2mm sin(2mx+40xt) %3D %3D 13) A bucket full of water hangs from one end of a string that passes over a light pulley. The other end of the string is driven by an oscillator of constant frequency, and the fundamental mode of standing waves is observed with one loop formed between the oscillatorand the pulley Holes are poked in the bucket causing it to start leaking water. When the bucket's mass drops to 1/4 of its initial value, oscillator pulley oscillator pulley kaking bucket water-filled
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