Lectures |
Table of Contents |
|
In the 1890's and early 1900's, astronomers methodically cataloged hundreds of thousands of stellar spectra. At Harvard, astronomer Annie Jump Cannon revised an older classification scheme, arranging the spectra according to the absorption line features -- especially the Balmer lines of hydrogen -- that they showed. Eventually it was realized that the differences in absorption lines were caused primarily by different temperatures at the surfaces of stars, and the spectral sequence was reordered by temperature.
Spectral types:
O B A F G K M
hot
cool
"oh be a fine gorilla: kiss me"
"oblique bats announce: frigid grapes kill mice"
Each 'spectral type' has a unique characteristic spectrum
| Spectral Type | Temperature (degrees Kelvin) | "Color" |
| O | 30,000 | blue/purple |
| B | 20,000 | blue |
| A | 10,000 | white |
| F | 8,000 | yellow/white |
| G | 6,000 | yellow |
| K | 4,000 | orange |
| M | 3,000 | red |
The greater the radial velocity (speed towards or away), the greater the shift. This means you can measure an object's speed towards or away from you by measuring the wavelength of features in its spectrum! In practice, this is done using absorption or emission lines (since continuum doesn't have any features to shift). For radial velocities (Vr) small compared to the speed of light (less than, say, 1% of c), the amount of shift in wavelength is given by:
![]() /
= Vr/c |

is the
change in
induced by the motion,
i.e.,
new -
old. (It gets a bit more complicated
for higher velocities.)
Lectures |
Table of Contents |
|