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Two simple harmonic motion are represrnt...

Two simple harmonic motion are represrnted by the following equation `y_(1) = 40 sin omega t` and `y_(2) = 10 (sin omega t + c cos omega t)`. If their displacement amplitudes are equal, then the value of `c` (in appropriate units) is

A

`sqrt(13)`

B

`sqrt (15)`

C

`sqrt (17)`

D

`4`

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To solve the problem, we need to find the value of \( c \) such that the displacement amplitudes of the two simple harmonic motions represented by the equations \( y_1 = 40 \sin(\omega t) \) and \( y_2 = 10 (\sin(\omega t) + c \cos(\omega t)) \) are equal. ### Step-by-Step Solution: 1. **Identify the Amplitudes**: - From the first equation \( y_1 = 40 \sin(\omega t) \), the amplitude \( A_1 \) is \( 40 \). - From the second equation \( y_2 = 10 (\sin(\omega t) + c \cos(\omega t)) \), we can rewrite it as: \[ y_2 = 10 \sin(\omega t) + 10c \cos(\omega t) \] - Here, the amplitude \( A_2 \) can be found using the formula for the resultant amplitude of two perpendicular components: \[ A_2 = \sqrt{(10)^2 + (10c)^2} = \sqrt{100 + 100c^2} = 10\sqrt{1 + c^2} \] 2. **Set the Amplitudes Equal**: - Since the problem states that the amplitudes are equal, we set \( A_1 = A_2 \): \[ 40 = 10\sqrt{1 + c^2} \] 3. **Solve for \( c \)**: - Divide both sides by 10: \[ 4 = \sqrt{1 + c^2} \] - Square both sides to eliminate the square root: \[ 16 = 1 + c^2 \] - Rearranging gives: \[ c^2 = 16 - 1 = 15 \] - Taking the square root of both sides: \[ c = \sqrt{15} \] 4. **Final Result**: - The value of \( c \) is \( \sqrt{15} \).

To solve the problem, we need to find the value of \( c \) such that the displacement amplitudes of the two simple harmonic motions represented by the equations \( y_1 = 40 \sin(\omega t) \) and \( y_2 = 10 (\sin(\omega t) + c \cos(\omega t)) \) are equal. ### Step-by-Step Solution: 1. **Identify the Amplitudes**: - From the first equation \( y_1 = 40 \sin(\omega t) \), the amplitude \( A_1 \) is \( 40 \). - From the second equation \( y_2 = 10 (\sin(\omega t) + c \cos(\omega t)) \), we can rewrite it as: \[ ...
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