The total power output of radiation emitted by a star, measured in Watts (W)
Radiant flux intensity F
The observed amount of intensity, or the radiant power transmitted normally through a surface per unit of area, of radiation measured on Earth
The luminosity is the total radiation that leaves the star
The radiant flux intensity is the amount of radiation measured on Earth
By the time the radiation reaches the Earth
It will have spread out a great deal, therefore, it will only be a fraction of the value of the luminosity
Inverse square law of flux
Light sources which are further away appear fainter because the light it emits is spread out over a greater area
Inverse square law of flux
The power from the star radiates uniformly through space
No radiation is absorbed between the star and the Earth
For a given star, the luminosity is constant
The radiant flux follows an inverse square law
The greater the radiant flux (larger F) measured, the closer the star is to the Earth (smaller d)
Worked example: Calculating distance from luminosity and radiant flux
1. Write down known quantities
2. Write down inverse square law of flux
3. Rearrange for distance d, and calculate
Standard candle
An astronomical object which has a known luminosity due to a characteristic quality possessed by that class of object
Examples of standard candles
Cepheid variable stars
Type 1a supernovae
Using standard candles as a distance indicator
If the luminosity of a source is known, then the distance can be estimated based on how bright it appears from Earth
Astronomers measure the radiant flux intensity of the electromagnetic radiation arriving at the Earth
Since the luminosity is known (as the object is a standard candle), the distance can be calculated using the inverse square law of flux
Collating the data and measurements from each standard candle method allows astronomers to build up a larger picture of the scale of the universe, known as the cosmic distance ladder
Wien's displacement law
The black body radiation curve for different temperatures peaks at a wavelength which is inversely proportional to the temperature
The higher the temperature of a body, the shorter the wavelength at the peak intensity, so hotter stars tend to be white or blue and cooler stars tend to be red or yellow
The higher the temperature of a body, the greater the intensity of the radiation at each wavelength
Worked example: Comparing surface temperatures of stars using Wien's law
1. Write down Wien's displacement law
2. Rearrange for temperature T
3. Calculate the surface temperature of each star
4. Conclude which star is cooler
Stefan-Boltzmann law
The total energy emitted by a black body per unit area per second is proportional to the fourth power of the absolute temperature of the body
Estimating the radius of stars
1. Use Wien's displacement law to find the surface temperature
2. Use the inverse square law of flux to find the luminosity
3. Use the Stefan-Boltzmann law to obtain the stellar radius
Estimating the radius of stars
1. Using Wien's displacement law to find the surface temperature of the star
2. Using the inverse square law of flux equation to find the luminosity of the star (if given the radiant flux and stellar distance)
3. Using the Stefan-Boltzmann law to obtain the stellar radius
Wien's displacement law
λ_max * T = 2.9 × 10^-3 m K
Calculating the surface temperature of Betelgeuse
Rearrange Wien's displacement law to find the surface temperature
Stefan-Boltzmann law
L = 4πr^2 σT^4
Calculating the stellar radius of Betelgeuse
Rearrange the Stefan-Boltzmann law to solve for r
The radius of Betelgeuse is about 1000 times larger than the Sun's radius
Astronomers are very limited in how they can investigate objects in space
All techniques used involve analysing the light emitted from the star or galaxy
One technique involves analysing the emission and absorption spectra of stars
Elements in the star, predominantly hydrogen and helium, absorb some of the emitted wavelengths
Characteristic lines are present when the spectrum is analysed
The top emission spectra shows spectral lines of hydrogen measured on Earth
The bottom emission spectra shows the shifted spectral lines of hydrogen measured from a distant galaxy
When astronomers observe light from distant galaxies, they observe differences in the spectral lines to the light from the Sun
The lines have the same characteristic pattern, meaning the element can still be easily identified, they just appear to be shifted slightly
The lines in the spectra from distant galaxies show an increase in wavelength
The lines are moved, or shifted, towards the red end of the spectrum
Doppler effect
The apparent change in wavelength or frequency of the radiation from a source due to its relative motion away from or toward the observer