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Sunspots and the rotation of the SunJosée SERT
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CAREFUL !
The observation of the Sun can turn out to be very dangerous, nobody must observe the Sun directly through an optical instrument (binoculars, telescope,...) without any protection. As the retina is not sensitive to pain, we can suffer irreversible injuries without noticing it at the very moment. On another hand, a long exposure of the instrument to the Sun may damage it seriously, even if filters are used. One of the only safe methods is to observe the Sun by projecting its image on a sheet of paper. See Figure 1.

With adhesive tape, fix a piece of light millimetered paper on the screen P after having drawn a 7 cm-radius circle on it (prepare several of them). Adjust the distance of the projection device so that the image of the Sun is the same size (or choose another radius for the circles). The difficulty is that the Earth is turning, and that the image of the Sun moves very fast. It is better to be two persons to do it : one who handles the instrument with flexibles, the other who plots the sunspots with a pencil.



You have to compute of what angle it moved : so, you draw the parallel, of which you can see a diameter [AB]. You can show the movement by drawing half a circle corresponding to the visible part of that parallel (its diameter [A'B']), then by drawing with perpendicular lines the positions of the spot from 1' to 4'. You can then measure the angle between the furthest positions.
That angle a corresponds to the duration d = t4 - t1 between the furthest plottings. You can then infer the synodic rotation period t (as seen from the Earth) :
To find the actual rotation period of the Sun T, you have to follow the argument written in the "Additional informations".
You have then :
(1 / t = (1 / T) - (1 / 365,25) , and you can find T knowing t .
Activity : (solution on Figure 4)

the A set (from A1 to A12) : March 1982 ;
the B set (from B1 to B7) : July 1982 ; A0 shows the equipment that was used.
The first slide in each set (i.e. slides 2 and 14) is a positive copy. The spots appear dark against a bright background. This is what students would see if they would observe an image of the Sun projected onto a screen. The following slides are negatives : they are direct copies of the negatives obtained with the equipment. For that reason, the details are crisper and more accurate.

a) Direction of rotation and position of the axis
If the slide has been correctly inserted in the projector, North is up and East is left. The successive positions of the spots show that the Sun's rotation is prograde (i.e. the visible part of the sphere rotates from East to West). The position of the rotational axis is determined by recording the motion of a spot over an interval of several days. In principle, its apparent part is an arc of ellipse except around two dates in the year, as the Equator of the Sun is tilted about 7° to the plane of the ecliptic : see Figure 6.

In fact, that arc of ellipse is very close to a chord. It is therefore possible to draw a line perpendicular to that chord going through the center. The angle between the axis so determined and the North-South axis is then measured with a protractor. Varying with the dates when the slides were exposed, the result is - 25° (March) and + 4° (July). See Figure 7. The angle is reckoned positively eastward from the North point of the Sun's disk.

b) We can of course determine the synodic period, then the sideral rotation period of the Sun as we did on the plotting papers.
c) More easily than on the plotting papers, we can see the differential rotation of the Sun : choose a spot located about the Equator, find its rotation period out, do the same thing with a spot the furthest from the Equator as possible, then compare.
The Sun is a sphere of gas in rotation around an axis, that rotation being faster in the equatorial areas than about the poles. It can be observed from the Earth only as the surface of the Sun shows details, the easiest to observe being the spots, that can be a marker ; we can measure the synodic period of rotation only, as the Earth is moving in relation to the Sun (see Figure 8).

After a sideral period T, the marker (a spot for example) comes back in the direction of the same star, but not in the direction of the Earth, as the Earth moved off. A little after, after a synodic period , the marker comes back in the direction of the Earth. After (in days), the Earth turned of an angle on its orbit, and the marker turned of (360° + ) on the surface of the Sun. So we have :
b = (360 x t ) / 365,25 on one hand and 360° + b = (360 x t ) / T on the other hand.
Hence (1 / t ) + (1 / 365,25) = 1 / T .
As we observe t , we compute T : so, as T varies from 25 to 29 days, we measure a period t from 26,8 days to 31,5 days from our observations.