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A particle is subjected to three SHM's i...

A particle is subjected to three SHM's in same direction simultaneously each having amplitude a and equal time period. The phase of the second motion is `30^(0)` ahead of the first and the phase of the third motion is `30^(0)` ahead of the second. Find the amplitude of the resultant motion.

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To find the amplitude of the resultant motion when a particle is subjected to three simple harmonic motions (SHMs) with the same amplitude and equal time period, we can follow these steps: ### Step 1: Define the SHMs Let the amplitude of each SHM be \( A \). The phases of the three SHMs are: - First SHM: \( \phi_1 = 0^\circ \) - Second SHM: \( \phi_2 = 30^\circ \) - Third SHM: \( \phi_3 = 60^\circ \) ### Step 2: Write the equations for each SHM The displacement for each SHM can be expressed in terms of their respective amplitudes and phases: - For the first SHM: \[ x_1 = A \cos(0^\circ) = A \] - For the second SHM: \[ x_2 = A \cos(30^\circ) = A \cdot \frac{\sqrt{3}}{2} \] - For the third SHM: \[ x_3 = A \cos(60^\circ) = A \cdot \frac{1}{2} \] ### Step 3: Calculate the resultant displacement The resultant displacement \( R \) can be found by summing the contributions from all three SHMs: \[ R = x_1 + x_2 + x_3 = A + A \cdot \frac{\sqrt{3}}{2} + A \cdot \frac{1}{2} \] Factoring out \( A \): \[ R = A \left( 1 + \frac{\sqrt{3}}{2} + \frac{1}{2} \right) \] ### Step 4: Simplify the expression Combine the terms inside the parentheses: \[ R = A \left( 1 + \frac{\sqrt{3} + 1}{2} \right) = A \left( \frac{2 + \sqrt{3} + 1}{2} \right) = A \left( \frac{3 + \sqrt{3}}{2} \right) \] ### Step 5: Calculate the amplitude of the resultant motion The amplitude of the resultant motion \( A_R \) is given by the magnitude of the resultant displacement: \[ A_R = \sqrt{R_x^2 + R_y^2} \] Where: - \( R_x = A \left( 1 + \frac{\sqrt{3}}{2} + \frac{1}{2} \right) \) - \( R_y = A \left( \frac{1}{2} + \frac{\sqrt{3}}{2} \right) \) Calculating \( R_x \) and \( R_y \): \[ R_x = A \left( \frac{3 + \sqrt{3}}{2} \right) \] \[ R_y = A \left( \frac{1 + \sqrt{3}}{2} \right) \] ### Step 6: Final expression for amplitude Now substituting back into the amplitude formula: \[ A_R = \sqrt{\left(A \cdot \frac{3 + \sqrt{3}}{2}\right)^2 + \left(A \cdot \frac{1 + \sqrt{3}}{2}\right)^2} \] \[ = A \cdot \frac{1}{2} \sqrt{(3 + \sqrt{3})^2 + (1 + \sqrt{3})^2} \] Calculating the squares: \[ (3 + \sqrt{3})^2 = 9 + 6\sqrt{3} + 3 = 12 + 6\sqrt{3} \] \[ (1 + \sqrt{3})^2 = 1 + 2\sqrt{3} + 3 = 4 + 2\sqrt{3} \] Adding these: \[ = (12 + 6\sqrt{3}) + (4 + 2\sqrt{3}) = 16 + 8\sqrt{3} \] Thus, the final amplitude of the resultant motion is: \[ A_R = A \cdot \frac{1}{2} \sqrt{16 + 8\sqrt{3}} \]
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RESONANCE-SIMPLE HARMONIC MOTION -Exercise- 1, PART - I
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