γεωμετρία = "earth measurement"
We rarely get a full, easily-understood description of a geometric object. Our information comes in two flavors: local and global.
The "puzzle piece" method
The "snapshot" method
Magellan/Elcano (1519-22)
On the Earth, all straight-line travel returns to the starting point after following a great circle.
The fundamental group records (in an algebraic form) the information about closed loops on a shape.
Magellan's path shows that, if you remove two points from the earth (the poles, for example) there is a non-trivial loop. With more mapping, we can conclude that there is really only one loop (which can be repeated some number of times.)
At different latitudes, observed angles of the sun and stars above the horizon are different.
The deviation of the curved surface from straight lines is measured by the second fundamental form.
Each point traces out a circular path once every 24 hours, with two exceptions -- the North and South poles.
It is crucial for studying immersions, or how the geometry of one geometric object relates to the geometry of another geometric space that contains it.
If one knows the distance to the ship d and the height of the mast h, one can calculate the radius of the Earth, R.
Around 200BC, the Greek geometer and librarian Eratosthenes calculated the circumference of the Earth.
Eratosthenes was measuring what we would now call the Gaussian curvature of the earth. The idea is to look at how fast the normal vectors to a surface change.
He knew that on the summer solstice, vertical objects in Syene cast no shadow, whereas to the north in Alexandria, they did.
positive curvature
Eratosthenes calculated the circumference of the Earth at 252,000 stadia.
The sun's rays are (approximately) parallel. Measuring the angle of the shadow in Alexandria told Eratosthenes that Alexandria --> Syene took up 1/50th of a full circle.
negative curvature
This is an error of 1.6% or 16.3%, depending on the stadia. With accurate data, the method has an error of about 66km, or .16%.
A dynamical system is a is some sort of movement or flow on our geometric object. The orbits are the paths that points trace out under this motion. The orbit structure of a rotating sphere distinguishes it from the examples here.
First demonstrated at the Pantheon in Paris in 1851, the plane of a pendulum's swing slowly rotates in relation to the floor.
The physics of this has to do with conservation of angular momentum.
The mathematical description for this process is parallel transport.
The angular momentum vector tries to stay pointing in the same direction, but must also be tangent to the Earth's surface.
For curved geometric objects, looking at parallel transport around closed loops is a great way to understand their geometry.
This forces it to rotate.
The angle sum for a triangle on the surface of the earth is not 180 degrees.
In fact it is always strictly more.
The relation between angles of a triangle and the radius of the earth is given by the Gauss-Bonnet Theorem.
Using the geodesic drawer at
http://geographiclib.sourceforge.net/scripts/geod-google.html
I drew a triangle connecting Taylor, Purdue, and IU. The angle discrepancy is .012 degrees, or .72'.