In the study of diffraction, particularly when discussing the diffraction of light through a single slit, we find the concept of maxima and minima. These are points where light is constructively or destructively interfering, respectively.
To deduce the expression for the diffraction maxima (often referred to as 'control maximum') for light passing through a single slit, we begin by understanding that maxima in a single-slit diffraction pattern occur where the light waves from different parts of the slit interfere constructively.
For a single slit of width a , the condition for maxima can be derived using the interference formula. In general, the position of the maxima in a single slit is given by the formula for minima instead, because these minima define the edges between which the maxima reside:
a sin θ = mλ
Here, a is the width of the slit, θ is the angle relative to the original direction of the light, m is the order of the minimum, and λ is the wavelength of the light. For a bright spot (secondary maximum) in between, these are approximated around values that do not satisfy the minimum condition. The exact locations and conditions for these secondary maxima are complex and usually require numerical methods for precise calculation or approximations.
Overall, the central maximum, the most intense region in the pattern, is located at θ = 0 , and the width of the central maximum can be expressed and understood by surrounding minima rather than unique conditions for maxima.
The presented formula focuses on finding minima because, for a slit, the calculation of secondary maxima is more complex, involving higher-level calculus and approximations around minima levels. For practical understanding, realizing where minima lie facilitates comprehension of visible maxima.