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Question: A sinusoidal wave has an amplitude of 3 cm, a time period of 1 s, and a wavelength of 1 cm. At x = 0...

A sinusoidal wave has an amplitude of 3 cm, a time period of 1 s, and a wavelength of 1 cm. At x = 0 and t = 0, the particle is at its mean position and moving upward. What is the equation of the wave if it is propagating in the positive x-direction?

A

y = 3cos(π\pi + 2π\pit - 2π\pix)

B

y = 3sin(2π\pit - 2π\pix)

C

y = 3sin(2π\pix - 2π\pit)

D

x = 3sin(2π\pit - 2π\piy)

Answer

y = 3sin(2π\pit - 2π\pix)

Explanation

Solution

The general equation of a sinusoidal wave propagating in the positive x-direction is given by:

y(x,t)=Asin(kxωt+ϕ)y(x, t) = A \sin(kx - \omega t + \phi)

where:

AA is the amplitude

kk is the wave number (k=2πλk = \frac{2\pi}{\lambda})

ω\omega is the angular frequency (ω=2πT\omega = \frac{2\pi}{T})

ϕ\phi is the phase constant

Given values:

Amplitude, A=3A = 3 cm

Time period, T=1T = 1 s

Wavelength, λ=1\lambda = 1 cm

  1. Calculate the wave number (kk):

k=2πλ=2π1 cm=2π cm1k = \frac{2\pi}{\lambda} = \frac{2\pi}{1 \text{ cm}} = 2\pi \text{ cm}^{-1}

  1. Calculate the angular frequency (ω\omega):

ω=2πT=2π1 s=2π rad/s\omega = \frac{2\pi}{T} = \frac{2\pi}{1 \text{ s}} = 2\pi \text{ rad/s}

  1. Substitute A, k, and ω\omega into the general wave equation:

y(x,t)=3sin(2πx2πt+ϕ)y(x, t) = 3 \sin(2\pi x - 2\pi t + \phi)

  1. Determine the phase constant (ϕ\phi) using the initial conditions:

At x=0x = 0 and t=0t = 0, the particle is at its mean position (y=0y = 0).

0=3sin(2π(0)2π(0)+ϕ)0 = 3 \sin(2\pi(0) - 2\pi(0) + \phi)

0=3sin(ϕ)0 = 3 \sin(\phi)

sin(ϕ)=0\sin(\phi) = 0

This implies ϕ=nπ\phi = n\pi, where nn is an integer. Possible values are 0,π,2π,...0, \pi, 2\pi, ....

At x=0x = 0 and t=0t = 0, the particle is moving upward. This means its velocity, yt\frac{\partial y}{\partial t}, is positive.

First, find the expression for the velocity:

yt=t[3sin(2πx2πt+ϕ)]\frac{\partial y}{\partial t} = \frac{\partial}{\partial t} [3 \sin(2\pi x - 2\pi t + \phi)]

yt=3cos(2πx2πt+ϕ)(2π)\frac{\partial y}{\partial t} = 3 \cos(2\pi x - 2\pi t + \phi) \cdot (-2\pi)

yt=6πcos(2πx2πt+ϕ)\frac{\partial y}{\partial t} = -6\pi \cos(2\pi x - 2\pi t + \phi)

Now, apply the condition at x=0,t=0x = 0, t = 0:

(yt)x=0,t=0=6πcos(2π(0)2π(0)+ϕ)>0(\frac{\partial y}{\partial t})_{x=0, t=0} = -6\pi \cos(2\pi(0) - 2\pi(0) + \phi) > 0

6πcos(ϕ)>0-6\pi \cos(\phi) > 0

cos(ϕ)<0\cos(\phi) < 0

Combining sin(ϕ)=0\sin(\phi) = 0 and cos(ϕ)<0\cos(\phi) < 0:

If ϕ=0\phi = 0, cos(ϕ)=1\cos(\phi) = 1 (not less than 0).

If ϕ=π\phi = \pi, cos(ϕ)=1\cos(\phi) = -1 (is less than 0).

Therefore, the phase constant ϕ=π\phi = \pi.

  1. Write the complete wave equation:

y(x,t)=3sin(2πx2πt+π)y(x, t) = 3 \sin(2\pi x - 2\pi t + \pi)

  1. Simplify the equation using trigonometric identities:

We know that sin(θ+π)=sin(θ)\sin(\theta + \pi) = -\sin(\theta).

So, y(x,t)=3sin(2πx2πt)y(x, t) = -3 \sin(2\pi x - 2\pi t)

We also know that sin(θ)=sin(θ)-\sin(\theta) = \sin(-\theta).

So, y(x,t)=3sin((2πx2πt))y(x, t) = 3 \sin(-(2\pi x - 2\pi t))

y(x,t)=3sin(2πt2πx)y(x, t) = 3 \sin(2\pi t - 2\pi x)

Therefore, the correct answer is y = 3sin(2π\pit - 2π\pix).