Solveeit Logo

Question

Question: In an experiment with sodium light ( \( 5890 A^o \) ), an interference pattern is obtained in which ...

In an experiment with sodium light ( 5890Ao5890 A^o ), an interference pattern is obtained in which 2020 equally spaced fringes occupy 2.30cm2.30cm on the screen. On replacing the sodium light with another monochromatic source, 3030 fringes occupy 2.80cm2.80cm on the screen. Find the wavelength of the light from the second source.

Explanation

Solution

To solve this question, we first need to find the fringe width in both the scenarios using the given information. Then, we need to equate fringe width with the wavelength of the light source in each case. Finally, equating the two equations, we will get our answer.
β=totalwidthnumberoffringes\beta = \dfrac{{total{\kern 1pt} {\kern 1pt} {\kern 1pt} width}}{{number{\kern 1pt} {\kern 1pt} {\kern 1pt} of{\kern 1pt} fringes}} where β\beta is the fringe width
β=λDd\beta = \dfrac{{\lambda D}}{d} where β\beta is the fringe width, DD is the distance between screen and slits and dd is the distance between the slits.

Complete answer:
According to the information given in the question
Case 11
number{\kern 1pt} {\kern 1pt} {\kern 1pt} of{\kern 1pt} fringes = 20 \\\ space{\kern 1pt} {\kern 1pt} {\kern 1pt} occupied = 2.30cm \\\
For light of wavelength λ1=5890A˚{\lambda _1} = 5890{\AA}

Case 22
number{\kern 1pt} {\kern 1pt} {\kern 1pt} of{\kern 1pt} fringes = 30 \\\ space{\kern 1pt} {\kern 1pt} {\kern 1pt} occupied = 2.80cm \\\
For light of wavelength λ2{\lambda _2}
Now, using the eq β=totalwidthnumberoffringes\beta = \dfrac{{total{\kern 1pt} {\kern 1pt} {\kern 1pt} width}}{{number{\kern 1pt} {\kern 1pt} {\kern 1pt} of{\kern 1pt} fringes}} for case 11 and 22 , we get
β1=2.320{\beta _1} = \dfrac{{2.3}}{{20}} ------(i)
β2=2.830{\beta _2} = \dfrac{{2.8}}{{30}} -------(ii)
Now, from the equation β=λDd\beta = \dfrac{{\lambda D}}{d} , where DD and dd are unchanged in both the cases, we get the equations
β1=λ1Dd{\beta _1} = \dfrac{{{\lambda _1}D}}{d} ---(iii)
β2=λ2Dd{\beta _2} = \dfrac{{{\lambda _2}D}}{d} ---(iv)
Then, dividing eq (iii) with eq (iv) , we get
β1β2=λ1Ddλ2Dd β1β2=λ1λ2  \Rightarrow \dfrac{{{\beta _1}}}{{{\beta _2}}} = \dfrac{{\dfrac{{{\lambda _1}D}}{d}}}{{\dfrac{{{\lambda _2}D}}{d}}} \\\ \Rightarrow \dfrac{{{\beta _1}}}{{{\beta _2}}} = \dfrac{{{\lambda _1}}}{{{\lambda _2}}} \\\
Now, substituting the respective values in their respective places, we get
2.3202.830=5890λ2 2.320×302.8=5890λ2 2.32.8×32=5890λ2  \Rightarrow \dfrac{{\dfrac{{2.3}}{{20}}}}{{\dfrac{{2.8}}{{30}}}} = \dfrac{{5890}}{{{\lambda _2}}} \\\ \Rightarrow \dfrac{{2.3}}{{20}} \times \dfrac{{30}}{{2.8}} = \dfrac{{5890}}{{{\lambda _2}}} \\\ \Rightarrow \dfrac{{2.3}}{{2.8}} \times \dfrac{3}{2} = \dfrac{{5890}}{{{\lambda _2}}} \\\
Now, switching the numerator and denominator on both sides, we have
2.82.3×23=λ25890 λ25890=2.82.3×23 λ2=5890×2.82.3×23 λ2=4780Ao  \Rightarrow \dfrac{{2.8}}{{2.3}} \times \dfrac{2}{3} = \dfrac{{{\lambda _2}}}{{5890}} \\\ \Rightarrow \dfrac{{{\lambda _2}}}{{5890}} = \dfrac{{2.8}}{{2.3}} \times \dfrac{2}{3} \\\ \Rightarrow {\lambda _2} = 5890 \times \dfrac{{2.8}}{{2.3}} \times \dfrac{2}{3} \\\ \Rightarrow {\lambda _2} = 4780{A^o} \\\
Therefore, the wavelength of the light from the second source is 4780Ao4780{A^o} .

Note:
In the given question, it is specified that only the source of light is changed. So, we infer that DD and dd remain unchanged and hence cancel each other out. Also, the space occupied by the fringes can be taken in mmmm or cmcm both as they cancel out each other. But, in case the values of DD and dd are specified, make sure to convert all of them either in mmmm or cmcm .