"It's gonna be a bright, bright sun-shiny day!"
Words to Begin With
- Horizon is the horizontal plane
that extends from the point where the observer is standing, to
infinity, straight through space. Since we're only working with
relatively short distances (compared to the Universe), a line
extending N-S will be quite sufficient.
- Altitude (A) is the angle of the
sun over the horizon. In this problem, we will be working with the sun
at noon, so it will either be over the N or S horizon.
- Zenith (Z) is the angle that the
sun is from directly overhead, and it is equal to 90-A. It, too, can
be over the S or N horizon, but there is little need to state it.
- Declination (D) is the latitude
at which the sun is directly overhead. It is always between 23.5 N and
23.5 S latitude, those occurring on the Solstices.
- Latitude (L) is the location N or
S of the equator at which the observer is located. (It is determined
by radii from the center of Earth at different angles to the equator.
If such an angle is swept along the surface of the planet, it draws a
circle.)
A Quick Lesson in Basic Geometry
Diagram A
In Diagram A above, CD and AB are
parallel, intersecting EF at G and H, respectively. Congruent (same) sets
of angles are: 1, 3, 5, and 7; and 2, 4, 6, and 8. This is because
opposite angles (ie: 1 and 3) are congruent (which is true for any 2
intersecting lines), and because same-side angles of parallel lines (ie: 3
and 7) are congruent.
I will refer to this as the SS (Same-Side)
theorem.
And the Rest is Simple Mathematics...
Honest, I'm not kidding about this! I couldn't
do these for the longest time, but I finally figured out how and where I
went wrong: I was trying to make these problems a lot harder than they
were! Just relax; they aren't that hard. Take it from someone who knows.
Three Possible Cases
Important Note: If you are given information
about D, and you know either L or A, you can get
whichever of them you do not have.
Case 1.
Case 1.
- Z as the sum of D and L,
from the SS Theorem.
- Z will therefore be larger than
both D and L.
- D and the observer are in
different hemispheres.
Case 2.
Case 2.
- L is the sum of D and Z,
from the SS theorem.
- L is greater than each D
and Z.
- D and the observer are in the
same hemisphere.
- The observer is farther from the equator
than D is.
Case 3.
Case 3.
- D is the sum of L and Z,
from the SS theorem.
- D is greater than each L
and Z.
- D and the observer are in the
same hemisphere.
- The observer is closer to the equator
than D is.
How 'Bout an Example?
Suppose it is the first day of summer, and the
sun is over 23.5 N, and you've just observed the sun at an altitude of 50
degrees over the S horizon. What's your latitude?
First, let's examine what we have as
information.
- Declination = 23.5 N.
- Altitude = 50 over S horizon.
Next, what can we infer?
- Zenith = 40.
- Since we have to look S to see the sun
with a declination over a line of N latitude, we must be further to
the N than the declination, and we are in the same hemisphere as the
declination.
- This is, therefore, a Case 2 situation.
Now, we solve for our latitude.
- D + Z = L; 23.5 + 40 = 63.5 N
(remember we said it is in the same hemisphere as the declination.)
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