At mean position:
\[ v_{\text{max}} = A \omega = 10 \Rightarrow \omega = \frac{10}{4} = \frac{5}{2} \]
Using the equation \( v = \omega \sqrt{A^2 - x^2} \) and \( v = 5 \):
\[ 5 = \frac{5}{2} \sqrt{4^2 - x^2} \]
Solving,
\[ \sqrt{A^2 - x^2} = 2 \Rightarrow x^2 = A^2 - 4 = 16 - 4 = 12 \]
Thus, \( x = \sqrt{12} \) and \( \alpha = 12 \).
A particle is executing simple harmonic motion with a time period of 3 s. At a position where the displacement of the particle is 60% of its amplitude, the ratio of the kinetic and potential energies of the particle is:
If \[ \frac{dy}{dx} + 2y \sec^2 x = 2 \sec^2 x + 3 \tan x \cdot \sec^2 x \] and
and \( f(0) = \frac{5}{4} \), then the value of \[ 12 \left( y \left( \frac{\pi}{4} \right) - \frac{1}{e^2} \right) \] equals to: