Motivation for tangent space

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The isomorphism between tangents and derivations is surprising! As is the fact it is a linear map. However with calculus one is not far from that definition already.

Motivating example

Let us take (informally, because cases where θ=π2 and r=0 must be treated carefully) the manifold of the plane. The reader should be familiar with polar coordinates (giving things as an angle and a distance from the origin, rather than x and y)

We will have two ways of looking at points, as (x,y) - traditionally, and (r,θ) where:

  • (r,θ)(rcos(θ),rsin(θ))
  • (x,y)(x2+y2,arctan(yx))


The line

Take the line y=mx+c, where m is the gradient and c is the intercept with the y axis, writing this we see the line can be given as:

Form First coord Second coord
x,y x=t y=mt+c
r,θ r=t2(m2+1)+2mct+c2 θ=arctan(m+ct)
Pure forms
Form map
Cartesian y=mx+c
Polar[1] r=|c|(m2+1)(tan(θ)m)2+2mtan(θ)m+1

These formulas are easily found from substitution.

Lines as seen in the polar coordinate plane

Some lines in polar coordinates, the y axis is the angle and the x radius
all these lines have gradient 1 (the gradient would just affect where r tends off towards infinity, which happens at pi/4 here) and from left to right, c=0.5, 1, 2 and 4

(See diagram on right) - notice that there are some "iffy" parts with lines (as seen above) - there's a discontinuity at the asymptote! - let us see how it is drawn to understand why.

Drawing the line y=x+1

Using the equation above we see:

  • r=|c|(m2+1)(tan(θ)m)2+2mtan(θ)m+1
    becomes
  • r=2(tan(θ)1)2+2tan(θ)1+1
    - this isn't that useful though.

Consider drawing the graph, the logic goes as follows:

  • θ=0 - well where can r actually be now? Undefined? If you graph the above, r=1
  • As θ increases, we keep drawing y=x1 - it grows faster and faster as we get near θ=π4
  • - r is undefined!
  • θ increases further - we now start to come back down, and we draw y=x+1, this keeps being drawn until:
  • θ=3π4 - we become undefined for r again
  • θ increases further - we draw more of y=x1, until we meet


Tangents

Let us go from tangents in (x,y) to tangents in (r,θ)


Using the notation of the charts for the smooth manifold of (upper quadrant) of the plane we can use the transition map:

  • (βα1):R2++R+×(0,π2)
  • (βα1):(x,y)(x2+y2,arctan(yx))

to go from the plane in terms of (x,y) to the (r,θ) "chart" of the plane.


Let us compute the Jacobian of this map (at the point (x,y):

Jac(βα1)=(rxryθxθy)=(xx2+y2yx2+y2yx2+y2xx2+y2)

Notes about dimensions

Unit wise:

(δrδxδrδyδθδxδθδy)×(δxδy)=(δrδxδx+δrδyδyδθδxδx+δθδyδy)=(δrδθ)

Calculating tangents

Where (u,v) is a column vector representing a tangent (in the sense of direction) in the (x,y) sense of the manifold we can compute the following:

(xx2+y2yx2+y2yx2+y2xx2+y2)×(uv)=(xx2+y2u+yx2+y2vyx2+y2u+xx2+y2v)


Notice that so far we have not mentioned any sort of "function", and this is linear! (at a point anyway)

Specific tangent

Take y=x+1, at x=1 we see dydx=1, that is to say the tangent at p=(1,2) is (1,1)p

Jac(βα1)(11)=(35515)
(using graphical calculator)

From this we see:

drdθ=35515=356.708 (4sf)


Using my graphical calculator I found:

ddt[|c|(m2+1)(tan(t)m)2+2mtan(t)m+1]|t=arctan(yx)6.708 (4sf)
where
  • m=1
  • c=1
  • (x,y)=p



TODO: get back to tangent space



References

  1. Jump up Polar equation of a line