Download presentation
Presentation is loading. Please wait.
1
Atomic Spectra Lab 1
2
Light If we pass light through a prism or diffraction grating, we can see the intensity as a function of wavelength.
3
Type of Spectrum Solids, liquids, and dense gases emit light of all wavelengths, without any gaps – or a continuous spectrum
4
Thin gases emit light of only a few wavelengths - an emission or bright line spectrum.
5
If there is a source of light behind it, a thin gas will absorb light of the same wavelengths it emits this is called an absorption or dark line spectrum.
7
Different Emission Line Spectra
H He C
8
Balmer lines each element generates its own unique set of wavelengths of emission or absorption Balmer studied the optical spectrum of hydrogen and found a pattern in the wavelengths of its emission lines
9
Periodic Table of Elements
11
Balmer series – set of visible lines in H spectrum
For H, the wavelengths are a simple formula reproduces these wavelengths λ (n) = (364.5 nm * ( n2 /n2 – 4)) where n = 3, 4, 5, …..
12
other scientists found similar patterns in other portions of the electromagnetic spectrum
13
Paschen series Paschen, in the infrared, measured lines with wavelengths which matched the series λ (n) = (820.5 nm * ( n2 /n2 – 9)) where n = 4, 5, 6, …..
14
Lyman series Lyman, in the ultraviolet, a series of lines with wavelengths corresponding to the series λ (n) = (91.1 nm * ( n2 /n2 – 1)) where n = 2, 3, 4, …..
15
In fact, scientists soon realized that hydrogen's spectrum could be broken down into a large number of series, each of which had wavelengths obeying a formula like Λ (n,k) = (limit) * ( n2 /n2 – k2)) where n=k+I, k+2,…. The Lyman series corresponds to k=1 with a limit of 91.1 nm, the Balmer series to k=2 with a limit of nm, and so forth
Similar presentations
© 2025 SlidePlayer.com. Inc.
All rights reserved.