
- A$\pi $
- B$\frac{{2\pi }}{3}$
- ✓$\frac{{\pi }}{2}$
- D$\frac{{3\pi }}{4}$

$=\mathrm{A}-\left(\frac{\sqrt{2}-1}{\sqrt{2}}\right) \mathrm{A}=\frac{\mathrm{A}}{\sqrt{2}}$
So phase of the particle which is going towards
$+x$ is $\phi_{1}=\frac{\pi}{4}$
and for other particle $\quad \phi_{2}=2 \pi-\pi / 4$
$=\frac{7 \pi}{4}$
Phase difference $=\frac{7 \pi}{4}-\frac{\pi}{4}=\frac{6 \pi}{4}=\frac{3 \pi}{2}$ or $\frac{\pi}{2}$
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A block is projected from the Point $A$ of inclined plane $A B$ along its surface with a velocity just sufficient to carry it to the top Point $B$ at a height $10 m$. After reaching the Point $B$ the block slides down on inclined plane $BC$. Time it takes to reach to the point $C$ from point $A$ is $t (\sqrt{2}+1) s$. The value of $t$ is........(use $g =10 m / s ^{2}$ )
