The astronomical unit (AU) is the average distance from the earth to the sun:
1 AU =1.5x10^11
The light year is the distance travelled by light in a vacuum in a year:
1 ly = 3x10^8 x (365x24x60x60)
1 ly = 9.46x10^15
Parallax is where the closer an object is to the viewer the faster it moves.
A parsec is the distance to a star that subtends an angle of one second at a distance of 1 AU.
luminosity is the total power radiated by a star.
intensity is the power radiated per unit area at the observer.
Brightness is a subjective scale of measurement ; how bright a star appears depends on both its distance and the power emitted at visible wavelengths . Brightness is measured n the Hipparchus scale. The faintest star visible with the naked eye from earth has a value of 6 ; the brightest is one.
Apparent magnitude;
the brightness of an astronomical body as seen from earth. An observer receives 100 times more light from a star with m = 1 than m = 6 . A difference of 1 is equal to an intensity ratio of 2.51. Stars can have a negative value m
Absolute magnitude:
The apparent magnitude an astronomical body would have if it was 10 pc from the observer with d in pc:
m-M = 5 log10 (d/10)
d < 10 pc , m<M
d > 10 pc , m> M
Transits- light curves show decrease / periodic variation in apparent magnitude.
radial velocity- orbiting planets cause stars to wobble , and light is blue and red shifted.
Hubbles law states that the universe is expanding - all galaxies are moving away from each other . with :
v = Hd
H = Hubble constant
1/H is approximate age of universe
Evidence for the big bang comes from Hubble's law , supported by cosmic microwave background radiation and helium production in the early universe.
Quasars:
emit all types of EM radiation
come from supermassive black holes in the centre of galaxies.
have very large powers
Doppler effect:
The frequency and wavelength detected depend on the relative velocity of the observer.
change in f / f = v/c
red shift := change in wavelength / frequency = -v/c
Stefan's law:
l max T = 2.9x10^-3 mk
T in kelvins
hotter stars appear white/blue , cooler stars appear red
Wiens displacement law:
P = sAT^4
T in kelvin and A in m^2
if star x and star y are at the same temperature , X will appear brighter if it has a larger area than y
Px / Py = Ax /Ay (Tx/Ty)^4
Supernovae show a sudden, huge increase in magnitude over days and are billions of times brighter than the sun. Type 1a supernovae are used as standard candles to work out distances , using the inverse square law.
Neutron stars are made of neutrons, are small with a huge density , similar to that of atomic nuclei.
Black holes have escape velocity which defines the event horizon : this implies a radius of Rs = 2GM / c^2 . They can produce gamma rays burst during formation and probably exist as supermassive black holes at the centre of galaxies.
Dark energy could be responsible for the accelerated expansion of the universe.
Stars are classified by temperatures O (hot , ionized) , B,A,F,G,K,M (cool).
above 10,000 K (O-A) - hydrogenis ionized
below 10,000 K (A-M) - electrons move up then down by different steps producing dimming = absorption lines.
Hipparchus scale:
1
2 x 2.5
3 x 6.25
4 x 16
5 x 40
6 x 100
To find brightness in from the hipparchus scale:
find the difference in hipparchus scale from two points
turn the difference into a power of 2.51
solve
luminosity is the total power radiated by a star (W)
Intensity is the power radiated per unit area at the observer (W/m^2)
Brightness is a subjective scale of measurement , how bright a star appears depends on both its distance and the power emitted at visible wavelength.
Apparent magnitude is the brightness of an astronomical scale as seen from earth (hipparchus scale).
Absolute magnitude is the apparent magnitude an astronomical body would have if it was 10pc from the observer.
How to find absolute magnitude:
m - M = 5 ln ( d/10 ) where d is in parsecs
If d is 10 parsecs then:
m-M = 5 ln (10/10)
m-M = 5 ln(1)
m-M = 0
Both magnitudes are equal
A black body is a body which absorbs all the radiation hitting it
Black body radiation is a type of e/m radiation which is emitted by a perfect black body which is held at a constant uniform temperature.
The spectrum peaks at a wavelength that shifts to shorter values at higher temperatures.
As the body gets hotter , more radiation is emitted ( the total power is proportional to the area under the graph), the spectrum applies to stars aswell.
Stefan's law states that total power P radiated by a body of surface area A is :
P = stefan's constant x surface area x temperature^4
Wien's law states that:
wavelength x temperature = 2.9x10^-3 mK
light emitted from the sun can produce a characteristic spectrum when viewed through a diffraction grating.
The absorption lines are produced when light passes through the cooler gases in the outer atmosphere of the sun.