As we will later learn, the entire energy generation of stars occurs through thermonuclear fusion in the stellar core. However, all of the energy that is generated in that core must escape the star, and hence if we can measure that escaping energy, we can infer the total energy generated.
In the case of Black body radiation, there is a straight forward relation between the energy generated (which is the total area under the Planck curve). This relation is of the form:
Rather than simply telling you the value of n, or having you look it up in a textbook or on the Internet, it is more instructive if you do a virtual experiment and actual measure this value. Then you will better understand the relation. The procedure for doing this is explained below. After you have tried this, you will be able to click on "the answer" so that you can confirm your measurement.
The simulation for this should appear below. The exercise here is fairly simple. If you drag the left (blue) or right (red) thermometers up to some temperature, the blackbody curve for that temperature will appear in the graph. The background graph is gridded into a number of boxes. If you count the boxes under the curve, that is the total area under the curve which is the total amount of energy emitted.
Experimental Procedure:
Now notice that the high temperature (9400) is 2 times larger than the low temperature (4700).
Refer back to the (Temp)n scaling relation. We have just increased the temperature by a factor of two, so the total energy emitted has now increased by 2n.
Before actually counting the boxes, it should be clear that the value of n must be large than 1. If n=1 then there would be twice as many boxes under the blue curve as under the red curve; clearly there are more than twice as many boxes under the blue curve.
You can then determine the value of