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Question: Two coherent point sources \({S}_{1}\) and \({S}_{2}\) vibrating in phase emit light of wavelength \...

Two coherent point sources S1{S}_{1} and S2{S}_{2} vibrating in phase emit light of wavelength λ\lambda. The separation between the sources is 2λ2\lambda. Consider a line passing through S2{S}_{2} and perpendicular to the line S1S2{S}_{1}{S}_{2}. What is the smallest distance from S2{S}_{2} where a minimum of intensity occurs?

Explanation

Solution

Here, the smallest distance for minimum intensity is asked i.e. dark fringe. So, the path difference of light from point sources must be equal to the path difference for dark fringe. Substitute the values in above mentioned relation and solve it to obtain the relation for distance between S2{S}_{2} and the point where fringes will be obtained. Now, assume the values of n=1,3,3 and so on and find the smallest distance.

Complete solution:

For minimum intensity of light, path difference of light from point sources must be equal to the path difference for dark fringe.
From the above figure, path difference is given by,
pathdifference=S1PS2Ppath \quad difference= {S}_{1}P – {S}_{2}P …(1)
Path difference for dark fringe is given by,
pathdifference=(2n+1)λ2path \quad difference= \left(2n+1 \right) \dfrac {\lambda}{2} …(2)
From the equation. (1) and (2) we get,
S1PS2P=(2n+1)λ2{S}_{1}P – {S}_{2}P= \left(2n+1 \right) \dfrac {\lambda}{2} …(3)
From the above figure we can say,
(S1P)2=(S1S2)2+(S2P)2{\left ({S}_{1}P\right )}^{2}= {\left({S}_{1}{S}_{2}\right)}^{2}+ {\left({S}_{2}P\right)}^{2}
Substituting values in above equation we get,
(S1P)2=(2λ)2+a2{\left({S}_{1}P\right)}^{2}= {\left(2 \lambda\right)}^{2}+ {a}^{2}
(S1P)2=4λ2+a2\Rightarrow {\left({S}_{1}P\right)}^{2}= 4 {\lambda}^{2}+ {a}^{2}
Taking the square root on both the sides we get,
S1P=4λ2+a2{S}_{1}P= \sqrt{4{ \lambda}^{2}+ {a}^{2}}
Now, substituting values in the equation. (3) we get,
4λ2+a2a=(2n+1)λ2\sqrt{4{ \lambda}^{2}+ {a}^{2}}-a= \left(2n+1 \right) \dfrac {\lambda}{2}
4λ2+a2=(2n+1)λ2+a\Rightarrow \sqrt{4{ \lambda}^{2}+ {a}^{2}}= \left(2n+1 \right) \dfrac {\lambda}{2}+a
Squaring both the sides we get,
4λ2+a2=(2n+1)2λ24+aλ(2n+1)+a24 {\lambda}^{2}+ {a}^{2}= { \left( 2n+1 \right) }^{ 2 }\dfrac { { \lambda }^{ 2 } }{ 4 } +a\lambda \left( 2n+1 \right) +{ a }^{ 2 }
4λ2=(2n+1)2λ24+aλ(2n+1)\Rightarrow 4 {\lambda}^{2}= { \left( 2n+1 \right) }^{ 2 }\dfrac { { \lambda }^{ 2 } }{ 4 } +a\lambda \left( 2n+1 \right)
Rearranging the above equation we get,
a=4λ2(2n+1)2λ24(2n+1)λa=\dfrac { 4{ \lambda }^{ 2 }-{ \left( 2n+1 \right) }^{ 2 }\dfrac { { \lambda }^{ 2 } }{ 4 } }{ \left( 2n+1 \right) \lambda }
a=16λ2(2n+1)2λ24(2n+1)λ\Rightarrow a=\dfrac { \dfrac { 16{ \lambda }^{ 2 }-{ \left( 2n+1 \right) }^{ 2 }{ \lambda }^{ 2 } }{ 4 } }{ \left( 2n+1 \right) \lambda }
a=16λ2(2n+1)2λ24(2n+1)λ\Rightarrow a=\dfrac { 16{ \lambda }^{ 2 }-{ \left( 2n+1 \right) }^{ 2 }{ \lambda }^{ 2 } }{ 4\left( 2n+1 \right) \lambda } …(4)
Case.1) If n=0 then, equation. (4) becomes,
a=15λ24λa=\dfrac { 15{ \lambda }^{ 2 } }{ 4\lambda }
a=15λ4\Rightarrow a=\dfrac { 15{ \lambda } }{ 4 }
Case.2) If n=1 then, equation. (4) becomes,
a=7λ22λa=\dfrac { 7{ \lambda }^{ 2 } }{ 2\lambda }
a=7λ2\Rightarrow a=\dfrac { 7{ \lambda } }{ 2 }
Case.3) If n=2 then, equation. (4) becomes,
a=9λ220λa=\dfrac { -9{ \lambda }^{ 2 } }{ 20\lambda }
a=9λ20\Rightarrow a=\dfrac { -9{ \lambda } }{ 20 }
Thus, the smallest distance for minimum intensity is 7λ2\dfrac { 7{ \lambda } }{ 2 }.

Note:
Here, we have not substituted n=3,4 and so on because the calculated values we obtained were negative. We know, distance can never be negative. Thus, we concluded the last positive value obtained for a as the smallest distance for minimum intensity. Also, students must remember what will be the path difference for maximum and minimum intensity. If the maximum intensity was asked then we would have considered the path difference for bright fringe as,
pathdifference=(2n1)λ2path \quad difference= \left(2n-1 \right) \dfrac {\lambda}{2}