Diffraction Gratings Paul Avery Dept. of Physics University of Florida PHY 2049 Paul Avery 1 Diffraction Gratings Analysis similar to double slit • Many slits instead of 2 • Slits still separated by distance d • Maxima again occur only for d sin θ = mλ • Maxima are much sharper Example: N = 4 (first maxima shown below) Grating N=4 d d m=1 λ 2λ d 3λ d 4λ θ L Waves Path difference is exactly 1 wavelength between slits As N increases, maxima occur at same location but sharper! Paul Avery 2 Diffraction Gratings Paul Avery 3 Diffraction Gratings Paul Avery 4 Diffraction Gratings Calculation of intensity • Basically a product of single slit and multiple slit formula • Let a = slit width, d = slit separation, N = # of slits 2 ⎛ sin α ⎞ ⎛ sin β ⎞ I = I max ⎜ ⎟ ⎜ ⎟ ⎝ α ⎠ ⎝ Nβ ⎠ α = π a sin θ / λ β = N π d sin θ / λ Paul Avery 5 2 Diffraction Gratings Gratings in astronomy: “Spectroscopy” • Use d sin θ = mλ to determine wavelength (θ measured) • Typically have N = 60,000 – 100,000!! • Sharp peaks allow closely spaced wavelengths to be resolved x Important for distinguishing element “signatures” x Find all the elements in a stellar spectrum Example: Wavelengths at 600 and 600.05 nm • Easily resolved with 60,000 slit grating • Poorly resolved with 15,000 slit grating • Too few slits ⇒ same location but lines too wide to tell apart Paul Avery 6 Diffraction Gratings Paul Avery 7 Diffraction Gratings Example: High resolution solar spectrum near sodium absorption lines Note: 1 nm = 10 Angstroms Sodium lines λ D1 = 589.54 nm λ D2 = 588.94 nm Paul Avery } Δλ = 0.60 nm 8 Diffraction Gratings