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A sinusoidal wave is traveling on a str...

A sinusoidal wave is traveling on a string with speed 40 cm/s. The displacement of the particle of the string at x = 10 cm varies with time according to
y = (5.0cm) sin`(1.0-4.0s^(-1))t)`The linear density of the string is 4.0 g/cm

A

the frequency of wave is 0.64 Hz

B

the wavelenght of the wave 63 cm

C

the tension in the string 0.064 N

D

the wave equation is y = (5.0cm) sin `(0.1x-(4.0s^(-1)t)`

Text Solution

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The correct Answer is:
To solve the problem step by step, we will analyze the given information and apply the relevant physics concepts. ### Given Data: - Speed of the wave, \( V = 40 \, \text{cm/s} \) - Displacement equation: \( y = (5.0 \, \text{cm}) \sin(1.0 - 4.0 \, \text{s}^{-1} \cdot t) \) - Linear density of the string, \( \mu = 4.0 \, \text{g/cm} \) ### Step 1: Identify Parameters from the Wave Equation The general form of a sinusoidal wave is given by: \[ y = y_m \sin(kx - \omega t) \] From the given equation, we can identify: - Amplitude, \( y_m = 5.0 \, \text{cm} \) - Angular frequency, \( \omega = 4.0 \, \text{s}^{-1} \) ### Step 2: Calculate the Wavenumber \( k \) The displacement equation can be rewritten as: \[ y = 5.0 \sin(1.0 - 4.0 t) \] From this, we can see that \( kx = 1.0 \) when \( t = 0 \). Therefore, we can set \( k = 1.0 \, \text{cm}^{-1} \). ### Step 3: Calculate the Frequency \( f \) The frequency \( f \) can be calculated using the formula: \[ f = \frac{\omega}{2\pi} \] Substituting the value of \( \omega \): \[ f = \frac{4.0}{2\pi} \approx 0.64 \, \text{Hz} \] ### Step 4: Calculate the Wavelength \( \lambda \) The relationship between wavenumber \( k \) and wavelength \( \lambda \) is given by: \[ k = \frac{2\pi}{\lambda} \] Rearranging gives: \[ \lambda = \frac{2\pi}{k} \] Substituting \( k = 1.0 \, \text{cm}^{-1} \): \[ \lambda = \frac{2\pi}{1.0} \approx 6.28 \, \text{cm} \approx 63 \, \text{cm} \] ### Step 5: Calculate the Tension \( T \) in the String Using the wave speed \( V \) and the linear density \( \mu \), we can find the tension \( T \) using the formula: \[ V = \sqrt{\frac{T}{\mu}} \] Rearranging gives: \[ T = \mu V^2 \] First, convert \( \mu \) from grams to kilograms: \[ \mu = 4.0 \, \text{g/cm} = 0.004 \, \text{kg/cm} = 0.004 \times 100 = 0.4 \, \text{kg/m} \] Now substituting \( V = 0.4 \, \text{m/s} \): \[ T = 0.004 \, \text{kg/cm} \cdot (0.4 \, \text{m/s})^2 = 0.004 \cdot 0.16 = 0.00064 \, \text{N} = 0.064 \, \text{N} \] ### Step 6: Verify the Wave Equation The wave equation can also be expressed as: \[ y = y_m \sin(kx - \omega t) \] Substituting \( y_m = 5.0 \, \text{cm} \), \( k = 1.0 \, \text{cm}^{-1} \), and \( \omega = 4.0 \, \text{s}^{-1} \): \[ y = 5.0 \sin(1.0 x - 4.0 t) \] ### Summary of Results: 1. Frequency \( f \approx 0.64 \, \text{Hz} \) 2. Wavelength \( \lambda \approx 63 \, \text{cm} \) 3. Tension \( T \approx 0.064 \, \text{N} \) 4. Wave equation \( y = 5.0 \sin(1.0 x - 4.0 t) \)
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