Displacement of a particle executing SHM can be expressed as x=a sin ωt+δAt t = 0, it is observed that the particle is at x=a2 and, moving along positive r-direction. Then δ could be:

# Displacement of a particle executing SHM can be expressed as At t = 0, it is observed that the particle is at $\mathrm{x}=\frac{\mathrm{a}}{2}$ and, moving along positive r-direction. Then $\mathrm{\delta }$ could be:

1. A

$\frac{\mathrm{\pi }}{3}$

2. B

$\frac{\mathrm{\pi }}{6}$

3. C

$\frac{5\mathrm{\pi }}{6}$

4. D

$\frac{\mathrm{\pi }}{4}$

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