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Physics
Two coherent waves are represented by y1=a1 cos ω t and y2=a2 sin ω t, superimposed on each other. The resultant intensity is proportional to
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Q. Two coherent waves are represented by $y_{1}=a_{1} \cos \omega t$ and $y_{2}=a_{2} \sin \omega t$, superimposed on each other. The resultant intensity is proportional to
Wave Optics
A
$\left(a_{1}+a_{2}\right)$
21%
B
$\left(a_{1}-a_{2}\right)$
12%
C
$\left(a_{1}^{2}+a_{2}^{2}\right)$
56%
D
$\left(a_{1}^{2}-a_{2}^{2}\right)$
11%
Solution:
As, $y_{1}=a_{1} \cos \omega t=a_{1} \sin \left(\omega t+90^{\circ}\right)$
and $y_{2}=a_{2} \sin \omega t$
$\therefore $ Phase difference $=\phi=90^{\circ}$
$R=\sqrt{a_{1}^{2}+a_{2}^{2}+2 a_{1} a_{2} \cos \phi}$
$=\sqrt{a_{1}^{2}+a_{2}^{2}}$
$\therefore $ Resultant intensity, $I\propto R^{2}$
$\Rightarrow I \propto\left(a_{1}^{2}+a_{2}^{2}\right)$