Two sinusoidal waves of wavelength A = 2/3 m and amplitude A = 6 cm and differing with their phase constant, are travelling to the right with same velocity v = 50 m/s. The resultant wave function y_res (x,t) will have the form: y_res (x,t) = 12(cm) cos(4/2) sin(150πx-3 πt+ φ/2). y_res (x,t) = 12(cm) cos(4/2) sin(3tx- 150rtt+p/2). %3D y_res (x,t) = 12(cm) cos(p/2) sin(3tx+150rt+p/2). %3D y_res (x,t) = 12(cm) cos(p/2) sin(3rx- 180tt+p/2). %3D

Classical Dynamics of Particles and Systems
5th Edition
ISBN:9780534408961
Author:Stephen T. Thornton, Jerry B. Marion
Publisher:Stephen T. Thornton, Jerry B. Marion
Chapter3: Oscillations
Section: Chapter Questions
Problem 3.27P
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Two sinusoidal waves of wavelength A =
2/3 m and amplitude A = 6 cm and
differing with their phase constant, are
travelling to the right with same
velocity v
50 m/s. The resultant wave
function y_res (x,t) will have the form:
y_res (x,t) = 12(cm) cos(4/2)
sin(150πx-3πt+ φ/2) .
y_res (x,t) = 12(cm) cos(4/2) sin(3nx-
150rtt+p/2).
y_res (x,t) = 12(cm) cos(4/2)
sin(3tx+150rtt+p/2).
y_res (x,t) = 12(cm) cos(p/2) sin(3nx-
180rtt+p/2).
y_res (x,t) = 12(cm) cos(4/2)
sin(150πx+3πt +φ/2) .
Page 2 of 2
Transcribed Image Text:Two sinusoidal waves of wavelength A = 2/3 m and amplitude A = 6 cm and differing with their phase constant, are travelling to the right with same velocity v 50 m/s. The resultant wave function y_res (x,t) will have the form: y_res (x,t) = 12(cm) cos(4/2) sin(150πx-3πt+ φ/2) . y_res (x,t) = 12(cm) cos(4/2) sin(3nx- 150rtt+p/2). y_res (x,t) = 12(cm) cos(4/2) sin(3tx+150rtt+p/2). y_res (x,t) = 12(cm) cos(p/2) sin(3nx- 180rtt+p/2). y_res (x,t) = 12(cm) cos(4/2) sin(150πx+3πt +φ/2) . Page 2 of 2
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