Harold Dennis Taylor and David Gill

Summary

Harold Dennis Taylor and David Gill 1911 Encyclopædia Britannica (1911)

It is clearly established that Hall was the first inventor of the achromatic telescope; but Dollond did not borrow the invention from Hall without acknowledgment in the manner suggested by Lalande. His discovery was beyond question an independent one. The whole history of his researches proves how fully he was aware of the conditions necessary for the attainment of achromatism in refracting telescopes, and he may be well excused if he so long placed implicit reliance on the accuracy of experiments made by so illustrious a philosopher as Newton.
Source: Wikisource

Harold Dennis Taylor and David Gill 1911 Encyclopædia Britannica (1911)

In its simplest form the telescope consists of a convex objective capable of forming an image of a distant object and of an eye-lens, concave or convex, by which the image so formed is magnified. When the axis of the eye-lens coincides with that of the object-glass, and the focal point of the eye-lens is coincident with the principal focus of the object-lens, parallel rays incident upon the object-glass will emerge from the eye-piece as parallel rays. These, falling in turn on the lens of the human eye, are converged by it and form an image on the retina.
Source: Wikisource

Harold Dennis Taylor and David Gill 1911 Encyclopædia Britannica (1911)

If we now attach to the polar axis a graduated circle D D, called the “hour circle,” of which the microscope or vernier R reads 0h when the declination axis is horizontal, we can obviously read off the hour angle from the meridian of any star to which the telescope may be directed at the instant of observation. If the local sidereal time of the observation is known, the right ascension of the star becomes known by adding the observed hour angle to the sidereal time if the star is west of the meridian, or subtracting it if east of the meridian.
Source: Wikisource

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