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Sinusoidal waves 5.00 cm in amplitude a...

Sinusoidal waves `5.00 cm ` in amplitude are to be transmitted along a string having a linear mass density equal to `4.00xx10^-2kg//m`. If the source can deliver a maximum power of `90W` and the string is under a tension of `100N`, then the highest frequency at which the source can operate is (take `pi^2=10`)

A

`45.3Hz`

B

`50Hz`

C

`30Hz`

D

`62.3Hz`

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The correct Answer is:
To solve the problem, we will follow these steps: ### Step 1: Understand the relationship between power, amplitude, frequency, and tension in a wave on a string. The power \( P \) transmitted by a sinusoidal wave on a string can be expressed as: \[ P = \frac{1}{2} \mu A^2 \omega^2 v \] where: - \( P \) = power (in watts) - \( \mu \) = linear mass density (in kg/m) - \( A \) = amplitude (in meters) - \( \omega \) = angular frequency (in radians/second) - \( v \) = wave speed (in m/s) ### Step 2: Find the wave speed \( v \). The wave speed \( v \) on a string under tension \( T \) is given by: \[ v = \sqrt{\frac{T}{\mu}} \] where \( T \) is the tension in the string. ### Step 3: Substitute \( v \) into the power equation. Now, substituting \( v \) into the power equation, we have: \[ P = \frac{1}{2} \mu A^2 \omega^2 \sqrt{\frac{T}{\mu}} \] This simplifies to: \[ P = \frac{1}{2} A^2 \omega^2 \sqrt{\mu T} \] ### Step 4: Solve for \( \omega \). Rearranging the equation to solve for \( \omega \): \[ \omega^2 = \frac{2P}{A^2 \sqrt{\mu T}} \] Taking the square root gives: \[ \omega = \sqrt{\frac{2P}{A^2 \sqrt{\mu T}}} \] ### Step 5: Find the frequency \( f \). The frequency \( f \) is related to angular frequency \( \omega \) by: \[ f = \frac{\omega}{2\pi} \] Substituting the expression for \( \omega \): \[ f = \frac{1}{2\pi} \sqrt{\frac{2P}{A^2 \sqrt{\mu T}}} \] ### Step 6: Substitute the values. Now we will substitute the given values into the equation: - \( P = 90 \, \text{W} \) - \( A = 5.00 \, \text{cm} = 0.05 \, \text{m} \) - \( \mu = 4.00 \times 10^{-2} \, \text{kg/m} \) - \( T = 100 \, \text{N} \) Substituting these values: \[ f = \frac{1}{2\pi} \sqrt{\frac{2 \times 90}{(0.05)^2 \sqrt{4.00 \times 10^{-2} \times 100}}} \] ### Step 7: Calculate \( \sqrt{4.00 \times 10^{-2} \times 100} \). Calculating the term inside the square root: \[ \sqrt{4.00 \times 10^{-2} \times 100} = \sqrt{4.00} = 2 \] ### Step 8: Substitute back into the frequency equation. Now substituting this back: \[ f = \frac{1}{2\pi} \sqrt{\frac{180}{(0.05)^2 \times 2}} \] Calculating \( (0.05)^2 = 0.0025 \): \[ f = \frac{1}{2\pi} \sqrt{\frac{180}{0.0025 \times 2}} = \frac{1}{2\pi} \sqrt{\frac{180}{0.005}} = \frac{1}{2\pi} \sqrt{36000} \] ### Step 9: Calculate \( \sqrt{36000} \). Calculating \( \sqrt{36000} \): \[ \sqrt{36000} = 60 \sqrt{10} \] ### Step 10: Final calculation for frequency. Now substituting this back: \[ f = \frac{1}{2\pi} \times 60 \sqrt{10} \] Using \( \pi^2 = 10 \): \[ f = \frac{60 \sqrt{10}}{2 \times 3.16} = \frac{60 \sqrt{10}}{6.28} \approx 30 \, \text{Hz} \] ### Final Answer: The highest frequency at which the source can operate is approximately \( 30 \, \text{Hz} \).

To solve the problem, we will follow these steps: ### Step 1: Understand the relationship between power, amplitude, frequency, and tension in a wave on a string. The power \( P \) transmitted by a sinusoidal wave on a string can be expressed as: \[ P = \frac{1}{2} \mu A^2 \omega^2 v \] ...
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