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Two audio speakers are kept some distanc...

Two audio speakers are kept some distance apart and are driven by the same amplifier system. A person is sitting at a place 6.0 m from one of the speakers and 6.4 m from the other. If the sound signal is continuously varied from 500 Hz to 5000 Hz, what are the frequencies for which there is a destructive interference at the place of the listener? Speed of sound in air` = 320 ms^-1`

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To solve the problem of finding the frequencies for which there is destructive interference at the listener's position, we will follow these steps: ### Step 1: Determine the Path Difference The listener is located 6.0 m from speaker S1 and 6.4 m from speaker S2. The path difference (Δd) can be calculated as: \[ \Delta d = d_2 - d_1 = 6.4 \, \text{m} - 6.0 \, \text{m} = 0.4 \, \text{m} \] ### Step 2: Condition for Destructive Interference For destructive interference to occur, the path difference must be an odd multiple of half the wavelength (λ): \[ \Delta d = \left(2n + 1\right) \frac{\lambda}{2} \] where \(n\) is an integer (0, 1, 2, ...). ### Step 3: Express Wavelength in Terms of Frequency The wavelength (λ) can be expressed using the speed of sound (v) and frequency (f): \[ \lambda = \frac{v}{f} \] Given that the speed of sound in air is \(v = 320 \, \text{m/s}\), we can substitute this into the equation for path difference: \[ 0.4 = \left(2n + 1\right) \frac{v}{2f} \] Substituting \(v\): \[ 0.4 = \left(2n + 1\right) \frac{320}{2f} \] This simplifies to: \[ 0.4 = \left(2n + 1\right) \frac{160}{f} \] ### Step 4: Rearranging to Find Frequency Rearranging the equation to solve for frequency \(f\): \[ f = \left(2n + 1\right) \cdot 400 \] ### Step 5: Finding Frequencies within the Given Range We need to find the values of \(f\) for \(n = 0, 1, 2, ...\) that lie within the range of 500 Hz to 5000 Hz. 1. For \(n = 0\): \[ f = (2 \cdot 0 + 1) \cdot 400 = 400 \, \text{Hz} \quad \text{(not in range)} \] 2. For \(n = 1\): \[ f = (2 \cdot 1 + 1) \cdot 400 = 1200 \, \text{Hz} \quad \text{(in range)} \] 3. For \(n = 2\): \[ f = (2 \cdot 2 + 1) \cdot 400 = 2800 \, \text{Hz} \quad \text{(in range)} \] 4. For \(n = 3\): \[ f = (2 \cdot 3 + 1) \cdot 400 = 3600 \, \text{Hz} \quad \text{(in range)} \] 5. For \(n = 4\): \[ f = (2 \cdot 4 + 1) \cdot 400 = 4400 \, \text{Hz} \quad \text{(in range)} \] 6. For \(n = 5\): \[ f = (2 \cdot 5 + 1) \cdot 400 = 5200 \, \text{Hz} \quad \text{(not in range)} \] ### Conclusion The frequencies for which there is destructive interference at the listener's position are: - 1200 Hz - 2800 Hz - 3600 Hz - 4400 Hz

To solve the problem of finding the frequencies for which there is destructive interference at the listener's position, we will follow these steps: ### Step 1: Determine the Path Difference The listener is located 6.0 m from speaker S1 and 6.4 m from speaker S2. The path difference (Δd) can be calculated as: \[ \Delta d = d_2 - d_1 = 6.4 \, \text{m} - 6.0 \, \text{m} = 0.4 \, \text{m} \] ...
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ALLEN-WAVES AND OSCILLATIONS-Part-1(Exercise-04)[A]
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