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 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 $v(0)$.
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 $t=0$:
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 $\sin(\omega t)$:
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.
Two simple harmonic motions, as shown below, are at right angles. They are combined to form lissajous figures.
$x(t) = A \sin (at + \delta)$
$y(t) = B \sin (bt)$
Identify the correct match below :

A piston of mass $M$ is hung from a massless spring whose restoring force law goes as $F= -kx^3$, where $k$ is the spring constant of appropriate dimension. The piston separates the vertical chamber into two parts, where the bottom part is filled with 'n' moles of an ideal gas. An external work is done on the gas isothermally (at a constant temperature $T$) with the help of a heating filament (with negligible volume) mounted in lower part of the chamber, so that the piston goes up from a height $L_0$ to $L_1$, the total energy delivered by the filament is : (Assume spring to be in its natural length before heating)