- #1
Eternal Sky
- 8
- 0
Homework Statement
The left-hand end of a long horizontal stretched cord oscillates transversely in SHM with frequency f = 250 Hz and amplitude 2.6 cm. The cord is under a tension of 140 N and has a linear density [tex]\mu[/tex] = 0.12 kg/m. At t = 0, the end of the cord has an upward displacement 1.6 cm and is falling. What is the velocity and acceleration at t = 2.0 seconds at a point on the string that is 1.00 m from the left-hand end?
Homework Equations
[tex]v_{y} = -D_{M} \omega \cos (kx - \omega t)[/tex]
[tex]v = \sqrt{\frac{F_{T}}{\mu}}[/tex]
[tex]v = \lambda f[/tex]
The Attempt at a Solution
I determined the wave velocity using the equation,
[tex]v = \sqrt{\frac{F_{T}}{\mu}} = \sqrt{\frac{140 N}{.12 kg/m}} = 34 m/s[/tex]
I used this to find the wavelength [tex]\lambda[/tex],
[tex]\lambda = \frac{v}{f} = \frac{34 m/s}{250 Hz} = 0.14 m[/tex]
So, in the equation for the velocity of the particle,
[tex]k = \frac{2\pi}{\lambda} = 45/m[/tex]
[tex]\omega = 2\pi f = 1570/s[/tex]
Therefore, the equation for the particle velocity should be,
[tex]v = -(0.026 m)(1570/s)\cos[(45/m)(1.00 m) - (1570/s)(2.0 s)][/tex]
[tex]v = 35 m/s[/tex]
However, the book says that the answer is 41 m/s. Can someone tell me what I am doing wrong? Any help would be appreciated.