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(A) The general equation for simple harmonic motion along the $Y$-axis is given by $y = y_0 + A' \sin(\omega t + \phi)$,where $y_0$ is the mean positi

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$A$

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(A) The general equation for simple harmonic motion along the $Y$-axis is given by $y = y_0 + A' \sin(\omega t + \phi)$,where $y_0$ is the mean position,$A'$ is the amplitude,and $\phi$ is the phase constant.Comparing the given equation $y = A \sin(\omega t) + B$ with the general form,we identify the mean position as $B$ and the amplitude as $A$.The amplitude represents the maximum displacement of the particle from its mean position.Thus,the amplitude of the simple harmonic motion is $A$.

List-$I$	List-$II$
$A$. $\sin^2 \omega t$	$I$. Periodic but not $SHM$ $(T = 2\pi/\omega)$
$B$. $\sin^3 \omega t$	$II$. Periodic but not $SHM$ $(T = \pi/\omega)$
$C$. $\sin \omega t + \cos \pi \omega t$	$III$. Non-periodic
$D$. $\cos \omega t + \cos 2\omega t$	$IV$. Periodic but not $SHM$ $(T = 2\pi/\omega)$

$A$ particle executing simple harmonic motion along the $Y$-axis has its motion described by the equation $y = A \sin(\omega t) + B$. The amplitude of the simple harmonic motion is

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