(a) We know that when any particle passes through its equilibrium position its velocity is maximum .ThusAnswer
$v_{max}=2 \ m/s$
In SHM $v_{max}=\pm\omega A$
Where $\omega$ is the angular frequency of SHM
Now given that $A=10^{-3} \ m$
$\omega =2/10^{-3} =2000 \ rad/sec$
Now frequency of oscillations
$f=\frac{\omega}{2\pi}$
=318.3 Hz
Again, Time period
$T=1/f= \pi \times 10^{-3} \ s$
(b)
Displacement of particle executing SHM is given by
$x=Acos{(}\omega t+\varphi)$
Given that initial phase $\varphi=0$ and $A=10^{-3} \ m$
Thus
$x=10^{-3}cos{(}2000t)$
Again, velocity of SHM is given by
$v=A\omega sin{\omega}t$
Putting all the values
$v=-2sin{(}2000t)$
(a) Given thatAnswer
$F=-\left(\frac{\pi^2}{16}\right)x $
We know that for SHM, force is given by
$F=-kx$
Where k is the force constant
Comparing SHM general equation with the given force equation
$k=\frac{\pi^2}{16}$
Now angular velocity in SHM is given by
$\omega=\sqrt{\frac{k}{m}}$
=> $\omega=\sqrt{\frac{\pi^2}{16m}}$
Now m=4 kg
$ \omega =\pi /8$
Now at t=2sec,x=0 (equilibrium position) we know that displacement of particle is SHM is given by
$x=Acos{(}\omega t+\varphi)$
Now $ \omega =\pi /8$
At t=2 x=0
$0=Acos{(}\frac{\pi}{8}*2+\varphi)$
Or $\varphi= \pi /4$
So equation of displacement
$x=Acos{(}\frac{\pi}{8}t+\frac{\pi}{4})$
Where A is the amplitude of SHM
(b) Velocity of SHM is
$v=-A\omega s i n{(}\omega t+\varphi)$
In this case,
$v=-A\frac{\pi}{8}sin{(}\frac{\pi}{8}t+\frac{\pi}{4})$
Given that t=4 sec v=4 m/sec
$4=-A\frac{\pi}{8}sin{(}\frac{\pi}{8}4+\frac{\pi}{4})$
$A=-32\frac{2^{1/2}}{\pi}m$
Here negative sign indicates that particle was moving with -x direction at 4 sec
Let O be the equilibrium position of particle. If P and Q are the two positions of the particles at distance $x_1$ and $x_2$ from O respectively, the velocity $u_1$ at the position P is given byAnswer
$u_1=\omega\sqrt{A^2-x_1^2}$ ---(1)
The velocity $u_2$ at position Q is given by
$u_2=\omega\sqrt{A^2-x_2^2}$ ----(2)
Squaring 1 and 2 and subtracting
$u_1^2-u_2^2=\omega^2(x_2^2-x_1^2)$
Or
$\omega=\sqrt{\frac{u_1^2-u_2^2}{x_2^2-x_1^2}}$
Hence the Time period
$T=2\pi\left[\frac{x_2^2-x_1^2}{u_1^2-u_2^2}\right]^{1/2}$
Mass of the cylinder (M) =SL ρAnswer
In equilibrium position
Weight of the cylinder =Weight of Liquid displaced
Mg=Vρ0g
So V=M/ ρ0
Let the cylinder is displaced by x from the mean position, then it will displace additional liquid of volume Sx.
So upward force action on the cylinder
$F= -Sx \rho _0g$
$Ma=-Sx \rho _0g$
$a=-(\frac{S\rho_0g}{M})x$
$a=-(\frac{S\rho_0g}{SL\rho})x$
$a=-\left(\frac{\rho_0g}{\rho L}\right)x$
Since a=-kx
So the motion is SHM
Time period of SHM
$T=2\pi\sqrt{\frac{\rho L}{\rho_0g}}$
(a) t=0 , ψ =+AAnswer
Equation (A)
$\psi(0)=Acos{(}\omega*0+\varphi)$
$\varphi=0$
Equation (B)
$\psi(0)=Asin{(}\omega*0+\varphi)$
(b) t=0 , ψ =-A
Equation (A)
$-A=\psi(0)=Acos{\varphi}$
$\varphi=\pi$
Equation (B)
$-A=\psi(0)=Asin{\varphi}$
$\varphi=\frac{3\pi}{2}$
(c) t=0, ψ =+A/2
Equation (A)
$-A/2=\psi(0)=Acos{\varphi}$
$\varphi=\pi/3$
Equation (B)
$-A/2=\psi(0)=Asin{\varphi}$
$\varphi=\frac{\pi}{6}$
On a planet, if a body dropped initial velocity (u = 0) from a height h and takes time t to reach the groundAnswer
then
$h=\frac {1}{2}g_p t^2$
or
$g_p=4 \ m/s^2$
Using
$T=2\pi \sqrt {\frac {L}{g}}$
T=3.14 sec