91Ó°ÊÓ

In a diffraction grating setup, the grating spacing, denoted as \(d\), is a key component in determining how light diffuses into different angles. Consider a grating that is 1.50 cm wide with 2400 parallel lines. Grating spacing indicates the distance between consecutive lines, and it is calculated by dividing the total width by the number of lines. Here, the width in meters is given by:

• 1.50 cm converted to meters: 0.015 m
• Number of lines: 2400

The formula to find the grating spacing is: \[d = \frac{0.015 \, \mathrm{m}}{2400} = 6.25 \times 10^{-6} \, \mathrm{m}\] This value of \(d\) determines how the incident light will be spread out. Smaller spacings result in larger diffraction angles, helping to identify different wavelengths precisely.

The diffraction condition governs the formation of maxima (constructive interference) in a diffraction pattern and is given by the equation:\[m \lambda = d \sin \theta\]

• \(m\) is the order of maximum, representing the number of wavelengths that fit into the path difference between adjacent slits.
• \(\lambda\) is the wavelength of the light being used.
• \(d\) is the grating spacing.
• \(\theta\) is the angle of diffraction, the angle at which the maxima are observed.

In this problem, the diffraction condition allows us to solve for the wavelength \(\lambda\) when other variables are known. Here, we know it is a third-order maximum, meaning \(m = 3\), with a diffraction angle of \(18.0^\circ\) and a previously determined \(d\). Understanding this condition is essential for figuring out how different wavelengths will appear at different angles, leading to the observation of color separation.

Calculating the wavelength in a diffraction grating experiment involves the application of the diffraction condition formula. To find the wavelength \(\lambda\), we rearrange the formula:\[\lambda = \frac{d \sin \theta}{m}\]Plug in the given and calculated values:

• \(d = 6.25 \times 10^{-6} \, \mathrm{m}\)
• \(\theta = 18.0^\circ\)
• \(m = 3\)

First, compute \(\sin(18^\circ)\) which is approximately 0.309:\[\lambda = \frac{6.25 \times 10^{-6} \, \mathrm{m} \times 0.309}{3}\]The calculated wavelength is:\[\lambda \approx 6.4375 \times 10^{-7} \, \mathrm{m}\]This is how light wavelengths are measured in such experiments, demonstrating the use of trigonometric functions to find unknowns in wave optics.

When studying diffraction patterns, maxima are labeled based on the order of their occurrence—first, second, third, and so on. A third-order maximum refers to the third instance of constructive interference in the pattern. The order \(m = 3\) in this scenario indicates that three full wavelengths fit into the path difference created by the grating.
The diffraction condition \(m \lambda = d \sin \theta\) plays a crucial role in determining the wavelength associated with each order. Each higher order involves wider angles for their maxima. This relationship helps in precisely characterizing the spectral components of the light source. It's the same principle that allows complex diffractive analyses in scientific research and industry applications. The higher the order, the more separation there is between individual components in the resulting spectrum.