Download
the blackbody simulator for this part
This simulator reproduces the blackbody spectrum as a function of temperature.
The X-axis is wavelength increasing to the right (decreasing energy per photon).
The Y-axis is the amount of energy emitted at that wavelength. Clicking anywhere on the graph
will indicate the wavelength (value of the X-axis) at location of the cursor. This is useful
when you need to identify the wavelength of the peak emission. A background
corresponding to the optical spectrum (the rainbow) is superposed on the blackbody curve
to ease in identification of color. Black means that our eyes can't see the light and NOT that the color is black!
Light with wavelength shorter than about 3200 angstroms does not penetrate our atmosphere. This is where the
ultraviolet region of the electromagnetic spectrum begins.
As you change the temperature (T) you will see the curve changing but you will also see the numerical values in the B-V V-R U-B and T fields changing. For this exercise we will only care about the values in the T and B-V fields.
Now click on the box that says "Draw Limits of Integration" -the white lines
that appear there represent filter band passes of standard astronomical filters.
As you can see, filters measure a "band" of wavelengths, not just one wavelength. Their
response isn't perfect either. See how they curve at the edges. This means that not all
of the light at the edges of the filter bandwidth are 100% transmitted.
To measure stellar temperatures, astronomers put filters in front of their
digital cameras and measure the flux ratio between the two filters. For
B (blue) and V (visual or green) this ratio is encoded as the index value B-V.
The lower that number, the hotter the star (more flux is emitted in the B filter
than the V filter. A value of B-V = 0.5 means that approximately the same
amount of energy is emitted in the blue filter as the green filter.
As you can see, the B-V index is a sensitive indicator of stellar surface temperature for stars with temperatures of around 6000 (like our Sun). However, for very hot stars B-V starts to lose its sensitivity to temperature simply because the B and V wavelength regions contain very little of the total energy flux of the star. We can verify this by doing the last situations and compare that to what was just done.