It is straightforward to determine the size of the Earth and the distance to the Moon without using a telescope. The methods have been known since the third century BCE. However, few astronomers have done this measurement from data they have taken. We use a gnomon to determine the latitude and longitude of South Bend, Indiana, and College Station, Texas, and determine the value of the radius of the Earth to be Rearth=6290 km, only 1.4% smaller than the known value. We use the method of Aristarchus and the size of the Earth’s shadow during the lunar eclipse of June 15, 2011 to estimate the distance to the Moon to be 62.3Rearth, 3.3% greater than the known mean value. We use measurements of the angular motion of the Moon against the background stars over the course of two nights, using a simple cross staff device, to estimate the Moon’s distance at perigee and apogee. We use simultaneous observations of asteroid 1996 HW1 obtained with small telescopes in Socorro, New Mexico, and Ojai, California, to obtain a value of the Astronomical Unit of (1.59±0.19)×108 km, about 6% too large. The data and methods presented here can easily become part of an introductory astronomy laboratory class.

1.
The “van of Eratosthenes,”refers to the Greek astronomer Eratosthenes (ca. 276–195 BCE) who obtained the first estimate of the Earth’s circumference from observations of the Sun’s elevation on the summer solstice from Alexandria and a town 7 to the south
.
2.
M.
Rowan-Robinson
,
The Cosmological Distance Ladder: Distance and Time in the Universe
(
W. H.Freeman
,
New York
,
1985
).
3.
O.
Gingerich
and
J. R.
Voelkel
, “
Tycho Brahe’s Copernican campaign
,”
J. Hist. Astron.
29
,
1
34
(
1998
).
4.
A.
Van Helden
, “
Measuring solar parallax: The Venus transits of 1761 and 1769 and their nineteenth-century sequels
,” in
Planetary Astronomy from the Renaissance to the Rise of Astrophysics, Part B: The Eighteenth and Nineteenth centuries
, edited by
R.
Taton
and
C.
Wilson
(
Cambridge U.P.
,
Cambridge
),
1995
, pp.
153
168
.
5.
Reference 2, p.
48
.
6.
A. G.
Riess
 et al., “
A 3% solution: Determination of the Hubble constant with the Hubble Space Telescope and Wide Field Camera 3
,”
Astrophys. J.
730
,
119
1
(
2011
).
7.
The Astronomical Almanac
(
Nautical Almanac Office
,
Washington, DC
,
2006
). For this article we also needed information from the 2008 and 2010 volumes.
8.
The celestial meridian is the imaginary line in the sky that separates the east half from the west half.For an observer in the northern hemisphere the meridian extends from the north point on the horizon through the North Celestial Pole, through the zenith and down to the south point on the horizon. An object such as the Sun is at its highest point above the horizon when it crosses the celestial meridian.At that moment the local apparent solar time is, by definition, exactly 12 noon
.
9.
If a vertical pointed stick is used, one obtains the elevation angle of the upper limb of the Sun. To find the elevation angle of the center of the Sun requires subtracting the angular radius of the Sun.
10.
Apparent solar time is related to the hour angle of the visible Sun in the sky.Due to the tilt of the Earth’s axis of rotation to the plane of its orbit and the Earth’s elliptical orbit, apparent solar time ranges from 14 min behind to 16 min ahead of mean solar time. Our watch time is mean solar time adjusted (by the longitude difference) to the nearest 15 line of longitude west of Greenwich, England. For example, Central Standard Time is for locations which are about 90 longitude west of Greenwich, or 6 h west.
11.
J.
J. Nassau
,
Practical Astronomy
(
McGraw-Hill
,
New York
,
1948
), pp.
36
37
.
12.
The New International Atlas
(
Rand McNally
,
Chicago
,
1980
).
13.
V.
Bekeris
 et al., “
Eratosthenes 2009/2010: An old experiment in modern times
,”
Astron. Educ. Rev.
10
,
010201
(
2011
).
14.
J.
Evans
,
The History and Practice of Ancient Astronomy
(
Oxford U.P.
,
New York
,
1998
), pp.
68
73
.
15.
A. N.
Cox
,
Allen’s Astrophysical Quantities
(
Springer
,
New York
,
2000
), pp.
308
, 340.
16.
G. J.
Toomer
,
Ptolemy’s Almagest
(
Springer-Verlag
,
Berlin
,
1984
), p.
254
.
17.
K.
Krisciunas
, “
Determining the eccentricity of the Moon’s orbit without a telescope
,”
Am. J. Phys.
78
,
834
838
(
2010
).
18.
See <www.slooh.com> for images of the lunar eclipse of 2011 June 15.
19.
G. J.
Toomer
, “
Hipparchus
,,” in
Dictionary of Scientific Biography
, edited by
C. G.
Gillespie
(
Scribner
,
New York
,
1981
).
20.
W. M.
Smart
,
Textbook on Spherical Astronomy
, 6th ed., revised by
R. M.
Green
(
Cambridge U.P.
,
Cambridge
,
1977
), pp.
200
202
.
21.
Reference 14, pp.
252
254
.
22.
The pattern for the device that slides up and down the yardstick was obtained from the University of Washington
, <www.astro.washington.edu/courses/labs/clearinghouse/labs/Skywatch/angles.html >.
23.
The JPL Horizons website is at <ssd.jpl.nasa.gov/horizons.cgi#top>.
24.
The website of the Digital Sky Survey is at <archive.stsci.edu/cgi-bin/dss_form>
.
25.
The software iraf is distributed by the National Optical Astronomy Observatory, which is operated by the Association of Universities for Research in Astronomy.
26.
Reference 20, pp.
209
210
.
27.
J.
Meeus
,
Astronomical Formulae for Calculators
, 4th ed. (
Willmann-Bell
,
Richmond, VA
,
1988
), pp.
125
130
.
28.
K.
Krisciunas
, “
A more complete analysis of the errors in Ulugh Beg’s star catalogue
,”
J. Hist. Astron.
24
,
269
280
(
1993
). Only Tycho Brahe (1546-1601), his engineers, and observers were able to design and use metal instruments that gave much more accurate results. Nine fundamental reference stars observed by Tycho and his observers are accurate to better than 1 arc min in right ascension and declination. See
J. L. E.
Dreyer
,
Tycho Brahe: A Picture of Scientific Life and Work in the Sixteenth Century
(
Peter Smith
,
Gloucester, MA
,
1977
), pp.
387
388
.
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