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The value of total mechanical energy of ...

The value of total mechanical energy of a particle is SHM is

A

Always constant

B

Depend on time

C

`(1)/(2)KA^(2)"cos"^(2)(omegat+phi)`

D

`(1)/(2)mA^(2)"cos"^(2)(omegat+phi)`

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To find the total mechanical energy of a particle in simple harmonic motion (SHM), we can follow these steps: ### Step 1: Understand the Energy Components In SHM, the total mechanical energy (E) is the sum of kinetic energy (KE) and potential energy (PE). ### Step 2: Write the Expressions for KE and PE The kinetic energy (KE) of a particle in SHM is given by: \[ KE = \frac{1}{2} k (A^2 - x^2) \] where \( k \) is the spring constant, \( A \) is the amplitude, and \( x \) is the displacement from the mean position. The potential energy (PE) is given by: \[ PE = \frac{1}{2} k x^2 \] ### Step 3: Write the Total Mechanical Energy The total mechanical energy (E) can be expressed as: \[ E = KE + PE \] Substituting the expressions for KE and PE: \[ E = \frac{1}{2} k (A^2 - x^2) + \frac{1}{2} k x^2 \] ### Step 4: Simplify the Expression Now, we simplify the expression: \[ E = \frac{1}{2} k (A^2 - x^2) + \frac{1}{2} k x^2 \] Combining the terms: \[ E = \frac{1}{2} k A^2 - \frac{1}{2} k x^2 + \frac{1}{2} k x^2 \] The \( -\frac{1}{2} k x^2 \) and \( +\frac{1}{2} k x^2 \) cancel each other out: \[ E = \frac{1}{2} k A^2 \] ### Step 5: Conclusion The total mechanical energy \( E \) in simple harmonic motion is: \[ E = \frac{1}{2} k A^2 \] This value is constant and does not depend on the displacement \( x \) or time \( t \). ### Final Answer The total mechanical energy of a particle in SHM is always constant. ---

To find the total mechanical energy of a particle in simple harmonic motion (SHM), we can follow these steps: ### Step 1: Understand the Energy Components In SHM, the total mechanical energy (E) is the sum of kinetic energy (KE) and potential energy (PE). ### Step 2: Write the Expressions for KE and PE The kinetic energy (KE) of a particle in SHM is given by: \[ KE = \frac{1}{2} k (A^2 - x^2) \] ...
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