HI all:

In the new edition of the BSS Bulletin (vol. 12, Feb. 2000) on page 51,
there is a sketch of an azmuthal (Dali) sundial by John Singleton titled: "A
Horizontal Dial with Equation of Time Built in".

I see a couple of differences in this drawing and similar dials previously
described by Art Carlson and Fer J. DeVires.  Note that the order of the 12
concentric date rings, from center to perimeter, is different.  In
Singleton's version they run from April in the center to March on the
perimeter.  In Fer's version, they run from December in the center to
January on the outside.  I might add that in Mayall pg. 181 there are only
six date rings with each ring serving for two months with December in the
center and January on the outside.  Apparently, ring order and number of
rings are not important. Am I correct?

Also, Singleton mentions that he uses an inclined gnomon equal to the
latitude, whereas Art, Fer, and Mayall suggest using a vertical rod of any
height with no nodus instead.  I can easily understand how the dial works
using a polar axis gnomon. But I can not understand how a vertical gnomon
would work.  Wouldn't a vertical rod have to have a nodus of specific height
and be located north of center to work (with the nodus lying on an imaginary
polar axis style) Apparently not, as Fer, Art, and Mayall place the rod in
the center.  

I know we discussed the Dali azmuthal dial before, but the type of gnomon
one can use still confuses me. How does a vertical rod with no nodus and no
set height, function just like a polar axis gnomon?

Can anyone explain this so that my thick head will understand?
Thanks,

John Carmichael       

Reply via email to