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Question

The motion of a mass on a spring, with spring constant K is as shown in figure. 

The equation of motion is given by $x(t) = A\sin\omega t+B\cos\omega t$ with $\omega=\sqrt{\frac{K}{m}}$. 

Suppose that at time $t = 0$, the position of mass is $x(0)$ and velocity $v(0)$, then its displacement can also be represented as $x(t) = C\cos(\omega t-\phi)$, where $C$ and $\phi$ are

The correct answer is
$C = \sqrt{\frac{v(0)^2}{\omega^2} + x(0)^2}$, $\phi = \tan^{-1}\left(\frac{v(0)}{x(0)\omega}\right)$

Mass on Spring Motion Equation Analysis

The motion of a mass on a spring is described by the equation $x(t) = A\sin(\omega t) + B\cos(\omega t)$. This solution explains how to represent this motion in the amplitude-phase form $x(t) = C\cos(\omega t - \phi)$, determining the expressions for amplitude $C$ and phase angle $\phi$ using initial conditions $x(0)$ and $v(0)$.

Deriving Amplitude and Phase Angle

Step 1: Determine coefficients $A$ and $B$ from initial conditions.

First, find the velocity equation by differentiating the position equation $x(t)$ with respect to time ($t$):

$v(t) = \frac{dx}{dt} = \frac{d}{dt}(A\sin(\omega t) + B\cos(\omega t)) = A\omega\cos(\omega t) - B\omega\sin(\omega t)$

Now, apply the given initial conditions at $t=0$:

  • For position: $x(0) = A\sin(0) + B\cos(0)$. Since $\sin(0)=0$ and $\cos(0)=1$, this simplifies to $x(0) = B$.
  • For velocity: $v(0) = A\omega\cos(0) - B\omega\sin(0)$. Since $\cos(0)=1$ and $\sin(0)=0$, this simplifies to $v(0) = A\omega$.

From these results, we find the coefficients $B = x(0)$ and $A = \frac{v(0)}{\omega}$.

Substituting these back into the original position equation gives the motion in terms of initial conditions:

$x(t) = \frac{v(0)}{\omega}\sin(\omega t) + x(0)\cos(\omega t)$

Step 2: Relate to the amplitude-phase form $x(t) = C\cos(\omega t - \phi)$.

The amplitude-phase form uses the cosine difference identity: $\cos(\alpha - \beta) = \cos\alpha\cos\beta + \sin\alpha\sin\beta$. Applying this:

$x(t) = C(\cos(\omega t)\cos\phi + \sin(\omega t)\sin\phi)$ $x(t) = (C\cos\phi)\cos(\omega t) + (C\sin\phi)\sin(\omega t)$

By comparing this expanded form with the equation derived in Step 1 ($x(t) = x(0)\cos(\omega t) + \frac{v(0)}{\omega}\sin(\omega t)$), we can equate the coefficients of $\cos(\omega t)$ and $\sin(\omega t)$:

  • Coefficient of $\cos(\omega t)$: $C\cos\phi = x(0)$
  • Coefficient of $\sin(\omega t)$: $C\sin\phi = \frac{v(0)}{\omega}$

Step 3: Calculate the amplitude $C$.

To find $C$, we square both equations from Step 2 and add them together:

$(C\cos\phi)^2 + (C\sin\phi)^2 = (x(0))^2 + \left(\frac{v(0)}{\omega}\right)^2$

Factor out $C^2$ and use the trigonometric identity $\cos^2\phi + \sin^2\phi = 1$:

$C^2(\cos^2\phi + \sin^2\phi) = x(0)^2 + \frac{v(0)^2}{\omega^2}$ $C^2(1) = x(0)^2 + \frac{v(0)^2}{\omega^2}$ $C^2 = x(0)^2 + \frac{v(0)^2}{\omega^2}$

Taking the square root (and assuming amplitude $C$ is non-negative), we get the expression for the amplitude:

$C = \sqrt{x(0)^2 + \frac{v(0)^2}{\omega^2}}$

Step 4: Calculate the phase angle $\phi$.

To find $\phi$, we divide the equation for $C\sin\phi$ by the equation for $C\cos\phi$ from Step 2:

$\frac{C\sin\phi}{C\cos\phi} = \frac{v(0)/\omega}{x(0)}$

The $C$ terms cancel out, and using $\frac{\sin\phi}{\cos\phi} = \tan\phi$:

$\tan\phi = \frac{v(0)}{x(0)\omega}$

Solving for $\phi$ gives the expression for the phase angle:

$\phi = \tan^{-1}\left(\frac{v(0)}{x(0)\omega}\right)$

The derived expressions for amplitude $C$ and phase angle $\phi$ are thus obtained.

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