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Measuring the unreachable

Nothing in this subject can be picked up, weighed or visited. Every number in it was inferred from an angle or a brightness.
0.321.03.210320.100.321.03.21032100316semi-major axis (AU)MercuryVenusEarthMarsJupiterSaturnUranusNeptuneslope 3/2 — P² ∝ a³period (years) Orbits

The law that links period to size, and weighs everything

Kepler found that the square of the period goes as the cube of the orbit. Newton found the constant of proportionality, and that constant is a mass — which is how every mass in astronomy has been obtained since.

barycentrethe line joining them always passes through it Gravitation

Neither body is still, and the wobble is how planets are found

A planet does not orbit its star. Both orbit a point between them, and the star's share of that motion is small, measurable, and the reason thousands of planets are known.

distant starsJanuaryJuly2 AU1.3 pc2p = 1.54″distance = 1 ÷ parallax in arcsecondsangles hugely exaggerated: the true angle here is a five-thousandth of a degree Starlight

The triangle that reaches the stars, and stops

Parallax is the only distance measurement in astronomy that assumes nothing. It is also the only one with a hard ceiling, and everything beyond that ceiling rests on it.

-20-100102030apparent magnitudethe Sunfull MoonVenus at its bestSiriusVega, by definitionthe naked-eye limita good amateur telescopea large ground-based surveythe deepest exposuresbrighter ←→ fainterfive magnitudes = ×100 in light Starlight

A scale that runs backwards, multiplies, and works

Brighter stars have smaller magnitudes, and five steps is a factor of a hundred. A scale invented by eye in the second century BC turned out to be logarithmic, because eyes are.

visible050010001500200000.20.40.60.811.2wavelength (nm)3000 K, peak 966 nm5800 K, peak 500 nm10000 K, peak 290 nmeach curve scaled to its own peak Starlight

Colour is a thermometer, and it reads across the galaxy

A star's colour gives its surface temperature, from two brightness measurements and no other information. It is the cheapest useful measurement in astronomy.

R = 0.01R☉R = 0.1R☉R = R☉R = 10R☉R = 100R☉giantssupergiantswhite dwarfs1M☉3M☉20M☉40M☉the Sun10−410−21102104106surface temperature (K), increasing to the leftluminosity, in solar units Stars

The diagram that sorted the stars, by plotting two things against each other

Plot brightness against colour for a few thousand stars and they do not scatter. They fall on a narrow band with two islands off it, and explaining that structure is most of stellar astronomy.

0.100.321.03.210320.011.0100100001000000mass (solar units)0.2M☉ → 0.01L☉1M☉ → 1L☉5M☉ → 391L☉20M☉ → 50,088L☉dashed: a pure slope of 3.5 Stars

Mass decides everything, by a power of three and a half

Two stars of the same mass are almost the same star. Double the mass and the output multiplies by eleven — which is why a modest range of masses produces a colossal range of stars.

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