H1 - rotation of the milky way (tangent method)
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most stars and gas in MW are flattened into an exponentially-decaying disk surrounding a bulge
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if any object with mass emits light, light will trace the mass
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it can be concluded that most of the mass is concentrated within a few kpc from the centre
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defining an encircling radius
above with the galactic mass is constant with radius, -
so, Keplerian rotation can be used to estimate the velocity profile of the galaxy at large radii
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equating the gravitational and centrifugal acceleration, so at
, the rotational curve of the galaxy is:

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measuring the rotation of MW is harder than for other galaxies as earth's own motion needs to be accounted for
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to reconstruct the rotation profile, Doppler shift in the spectra of stars, HII regions, HI, CO, etc can be measured
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any measured Doppler shift can be converted into a radial component along the line of sight of the velocity
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these then need to be converted into orbital velocities
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using geometry to solve for all the orbital components internal to the orbit of the sun is called the tangent method
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geometrically:
- using the sine rule on the triangle defined by the sun, the object, and the galactic centre:
where,
- moving along the line of sight to the point where
, ie. the line of sight is tangent to the orbit:
- unless the rotational velocity increases with radius, the maximum radial velocity along the line of sight is measured at the tangent:
- note that the tangent point is only defined for
, limiting the method to galactic longitudes to between and - so, beyond sun's orbit, estimates of the rotational curve rely on different distance methods, and are more subject to uncertainty