\( \frac{2\pi \lambda}{a}\)
\( \frac{2\pi a}{\lambda}\)
\( \frac{\lambda}{a}\)
\( \frac{a}{\lambda}\)
The general equation for a travelling wave is:
y = A sin(kx − ωt)
where:
A is the amplitude.
k is the wave number ($k = \frac{2\pi}{\lambda}$).
ω is the angular frequency ($\omega = 2\pi f$).
f is the frequency.
Comparing this with given equation: y = C sin($\frac{2\pi}{\lambda}$(at − x)), we get ω = $\frac{2\pi a}{\lambda}$.
Since ω = 2πf: 2πf = $\frac{2\pi a}{\lambda}$
$f = \frac{a}{\lambda}$
A bob of heavy mass \(m\) is suspended by a light string of length \(l\). The bob is given a horizontal velocity \(v_0\) as shown in figure. If the string gets slack at some point P making an angle \( \theta \) from the horizontal, the ratio of the speed \(v\) of the bob at point P to its initial speed \(v_0\) is :