A particle executing SHM along a straight line has zero velocity at points \(A\) and \(B\) whose distance…
- \(\frac{\pi(b+a)}{v}\)
- \(\pi\left(\frac{b-a}{v}\right)\)
- \(\left(\frac{b+a}{2 v}\right)\)
- \(\left(\frac{b-a}{2 v}\right)\)
Solution

\(\therefore\) Amplitude \(=\frac{\text { Distance travelled by the particles }}{2}(A \text { to } B)\) Amplitude of particles executing simple harmonic motion (SHM) along a straight line \(A B\) is \((a)=\frac{b-a}{2}\). Velocity of particle, \(v=\) Amplitude \(\times\) Oscillation frequency \(\begin{aligned} \therefore \quad v & =a \omega \\ v & =\left(\frac{b-a}{2}\right) \omega \text { or } \omega=\frac{2 v}{b-a} \quad \ldots (i) \end{aligned}\) \(\therefore\) Time period, \(T=\frac{2 \pi}{\omega}\) Putting the value of \(\omega\) from Eq. (i) to above formula, \(\Rightarrow \quad T=\frac{2 \pi}{2 v} \times(b-a) \Rightarrow T=\frac{b-a}{v} \pi\) So, the time period of a particle executing SHM along a straight line from points \(A\) to \(B\) is, \(T=\frac{b-a}{v} \pi\)
Asked in: AP EAMCET 2019 (22 Apr Shift 1)