Difference between revisions of "Motivation for tangent space"

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(Created page with "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. ==Motiva...")
 
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These formulas are easily found from substitution.  
 
These formulas are easily found from substitution.  
  
{{Todo|Add picture, talk about tangents between the two!}}
+
==Lines as seen in the polar coordinate plane==
 +
[[Image:LinesInPolar.png|thumb|Some lines in polar coordinates, the y axis is the angle and the x radius<br/>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:
 +
* <math>r=|c|\sqrt{\frac{(m^2+1)}{(\tan(\theta)-m)^2}+\frac{2m}{\tan(\theta)-m}+1}</math> becomes
 +
* <math>r=\sqrt{\frac{2}{(\tan(\theta)-1)^2}+\frac{2}{\tan(\theta)-1} + 1}</math> - this isn't that useful though.
 +
 
 +
Consider drawing the graph, the logic goes as follows:
 +
* {{M|1=\theta=0}} - well where can {{M|r}} actually be now? Undefined? If you graph the above, {{M|1=r=1}}
 +
* As {{M|\theta}} increases, we keep drawing {{M|1=y=x-1}} - it grows faster and faster as we get near {{M|1=\theta=\tfrac{\pi}{4} }}
 +
* {{M|\theta=\tfrac{\pi}{4} }} - {{M|r}} is undefined!
 +
* {{M|\theta}} increases further - we now start to come back down, and we draw {{M|1=y=x+1}}, this keeps being drawn until:
 +
* {{M|1=\theta=\tfrac{3\pi}{4} }} - we become undefined for {{M|r}} again
 +
* {{M|\theta}} increases further - we draw more of {{M|1=y=x-1}}, until we meet {{M|\theta=0}}
 +
 
 +
 
 +
==Tangents==
 +
Let us go from tangents in {{M|(x,y)}} to tangents in {{M|(r,\theta)}}
 +
 
 +
 
 +
Using the notation of [[Motivation for smooth manifolds#Our charts|the charts for the smooth manifold of (upper quadrant) of the plane]] we can use the transition map:
 +
* <math>(\beta\circ\alpha^{-1}):\mathbb{R}^2_++\rightarrow\mathbb{R}_+\times(0,\tfrac{\pi}{2})</math>
 +
* <math>(\beta\circ\alpha^{-1}):(x,y)\mapsto\left(\sqrt{x^2+y^2},\arctan\left(\frac{y}{x}\right)\right)</math>
 +
to go from the plane in terms of {{M|(x,y)}} to the {{M|(r,\theta)}} "chart" of the plane.
 +
 
 +
 
 +
Let us compute the [[Jacobian]] of this map (at the point {{M|(x,y)}}:
 +
: <math>\text{Jac}(\beta\circ\alpha^{-1})=\begin{pmatrix}
 +
\frac{\partial r}{\partial x} & \frac{\partial r}{\partial y} \\
 +
\frac{\partial \theta}{\partial x} & \frac{\partial \theta}{\partial y}
 +
\end{pmatrix}=\begin{pmatrix}
 +
\frac{x}{\sqrt{x^2+y^2}} & \frac{y}{\sqrt{x^2+y^2}} \\
 +
\frac{-y}{x^2+y^2} & \frac{x}{x^2+y^2}
 +
\end{pmatrix}</math>
 +
 
 +
===Notes about dimensions===
 +
Unit wise:
 +
 
 +
<math>\begin{pmatrix}
 +
\frac{\delta r}{\delta x} & \frac{\delta r}{\delta y} \\
 +
\frac{\delta \theta}{\delta x} & \frac{\delta \theta}{\delta y}
 +
\end{pmatrix}\times\begin{pmatrix}
 +
\delta x \\ \delta y
 +
\end{pmatrix}=
 +
\begin{pmatrix}
 +
\frac{\delta r}{\delta x}\delta x + \frac{\delta r}{\delta y}\delta y \\
 +
\frac{\delta \theta}{\delta x}\delta x + \frac{\delta \theta}{\delta y}\delta y
 +
\end{pmatrix}=\begin{pmatrix}
 +
\delta r \\ \delta \theta
 +
\end{pmatrix}</math>
 +
===Calculating tangents===
 +
Where {{M|(u,v)}} is a column vector representing a tangent (in the sense of direction) in the {{M|(x,y)}} sense of the manifold we can compute the following:
 +
 
 +
: <math>\begin{pmatrix}
 +
\frac{x}{\sqrt{x^2+y^2}} & \frac{y}{\sqrt{x^2+y^2}} \\
 +
\frac{-y}{x^2+y^2} & \frac{x}{x^2+y^2}
 +
\end{pmatrix}\times\begin{pmatrix}
 +
u \\
 +
v
 +
\end{pmatrix}=\begin{pmatrix}
 +
\frac{x}{\sqrt{x^2+y^2}}u+\frac{y}{\sqrt{x^2+y^2}}v \\
 +
\frac{-y}{x^2+y^2}u+\frac{x}{x^2+y^2}v
 +
\end{pmatrix}</math>
 +
 
 +
 
 +
Notice that so far we have not mentioned any sort of "function", and this is linear! (at a point anyway)
 +
 
 +
====Specific tangent====
 +
Take {{M|1=y=x+1}}, at {{M|1=x=1}} we see {{M|1=\frac{dy}{dx}=1}}, that is to say the tangent at {{M|1=p=(1,2)}} is {{M|(1,1)_p}}
 +
 
 +
: <math>\text{Jac}(\beta\circ\alpha^{-1})\begin{pmatrix}
 +
1 \\ 1 \end{pmatrix} = \begin{pmatrix}
 +
\frac{3\sqrt{5}}{5} \\ \frac{-1}{5}
 +
\end{pmatrix}</math> (using graphical calculator)
 +
 
 +
From this we see:
 +
: <math>\frac{dr}{d\theta}=\frac{\frac{3\sqrt{5}}{5}}{\frac{-1}{5}}=-3\sqrt{5}\approx-6.708\text{ (4sf)}</math>
 +
 
 +
 
 +
Using my graphical calculator I found:
 +
 
 +
: <math>\left.\frac{d}{dt}\left[
 +
|c|\sqrt{\frac{(m^2+1)}{(\tan(t)-m)^2}+\frac{2m}{\tan(t)-m}+1}
 +
\right]\right|_{t=\arctan(\frac{y}{x})}\approx -6.708\text{ (4sf)}</math>
 +
: where
 +
:* {{M|1=m=1}}
 +
:* {{M|1=c=1}}
 +
:* {{M|1=(x,y)=p}}
 +
 
 +
{{Todo| get back to tangent space}}
  
 
==References==
 
==References==

Latest revision as of 00:18, 11 April 2015

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 [ilmath]\theta=\tfrac{\pi}{2}[/ilmath] and [ilmath]r=0[/ilmath] 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 [ilmath]x[/ilmath] and [ilmath]y[/ilmath])

We will have two ways of looking at points, as [ilmath](x,y)[/ilmath] - traditionally, and [ilmath](r,\theta)[/ilmath] where:

  • [ilmath](r,\theta)\mapsto(r\cos(\theta),r\sin(\theta))[/ilmath]
  • [ilmath](x,y)\mapsto\left(\sqrt{x^2+y^2},\arctan(\frac{y}{x})\right)[/ilmath]


The line

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

Form First coord Second coord
[ilmath]x,y[/ilmath] [ilmath]x=t[/ilmath] [ilmath]y=mt+c[/ilmath]
[ilmath]r,\theta[/ilmath] [ilmath]r=\sqrt{t^2(m^2+1)+2mct+c^2}[/ilmath] [ilmath]\theta=\arctan\left(m+\frac{c}{t}\right)[/ilmath]
Pure forms
Form map
Cartesian [ilmath]y=mx+c[/ilmath]
Polar[1] [math]r=|c|\sqrt{\frac{(m^2+1)}{(\tan(\theta)-m)^2}+\frac{2m}{\tan(\theta)-m}+1}[/math]

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:

  • [math]r=|c|\sqrt{\frac{(m^2+1)}{(\tan(\theta)-m)^2}+\frac{2m}{\tan(\theta)-m}+1}[/math] becomes
  • [math]r=\sqrt{\frac{2}{(\tan(\theta)-1)^2}+\frac{2}{\tan(\theta)-1} + 1}[/math] - this isn't that useful though.

Consider drawing the graph, the logic goes as follows:

  • [ilmath]\theta=0[/ilmath] - well where can [ilmath]r[/ilmath] actually be now? Undefined? If you graph the above, [ilmath]r=1[/ilmath]
  • As [ilmath]\theta[/ilmath] increases, we keep drawing [ilmath]y=x-1[/ilmath] - it grows faster and faster as we get near [ilmath]\theta=\tfrac{\pi}{4}[/ilmath]
  • - [ilmath]r[/ilmath] is undefined!
  • [ilmath]\theta[/ilmath] increases further - we now start to come back down, and we draw [ilmath]y=x+1[/ilmath], this keeps being drawn until:
  • [ilmath]\theta=\tfrac{3\pi}{4}[/ilmath] - we become undefined for [ilmath]r[/ilmath] again
  • [ilmath]\theta[/ilmath] increases further - we draw more of [ilmath]y=x-1[/ilmath], until we meet


Tangents

Let us go from tangents in [ilmath](x,y)[/ilmath] to tangents in [ilmath](r,\theta)[/ilmath]


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

  • [math](\beta\circ\alpha^{-1}):\mathbb{R}^2_++\rightarrow\mathbb{R}_+\times(0,\tfrac{\pi}{2})[/math]
  • [math](\beta\circ\alpha^{-1}):(x,y)\mapsto\left(\sqrt{x^2+y^2},\arctan\left(\frac{y}{x}\right)\right)[/math]

to go from the plane in terms of [ilmath](x,y)[/ilmath] to the [ilmath](r,\theta)[/ilmath] "chart" of the plane.


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

[math]\text{Jac}(\beta\circ\alpha^{-1})=\begin{pmatrix} \frac{\partial r}{\partial x} & \frac{\partial r}{\partial y} \\ \frac{\partial \theta}{\partial x} & \frac{\partial \theta}{\partial y} \end{pmatrix}=\begin{pmatrix} \frac{x}{\sqrt{x^2+y^2}} & \frac{y}{\sqrt{x^2+y^2}} \\ \frac{-y}{x^2+y^2} & \frac{x}{x^2+y^2} \end{pmatrix}[/math]

Notes about dimensions

Unit wise:

[math]\begin{pmatrix} \frac{\delta r}{\delta x} & \frac{\delta r}{\delta y} \\ \frac{\delta \theta}{\delta x} & \frac{\delta \theta}{\delta y} \end{pmatrix}\times\begin{pmatrix} \delta x \\ \delta y \end{pmatrix}= \begin{pmatrix} \frac{\delta r}{\delta x}\delta x + \frac{\delta r}{\delta y}\delta y \\ \frac{\delta \theta}{\delta x}\delta x + \frac{\delta \theta}{\delta y}\delta y \end{pmatrix}=\begin{pmatrix} \delta r \\ \delta \theta \end{pmatrix}[/math]

Calculating tangents

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

[math]\begin{pmatrix} \frac{x}{\sqrt{x^2+y^2}} & \frac{y}{\sqrt{x^2+y^2}} \\ \frac{-y}{x^2+y^2} & \frac{x}{x^2+y^2} \end{pmatrix}\times\begin{pmatrix} u \\ v \end{pmatrix}=\begin{pmatrix} \frac{x}{\sqrt{x^2+y^2}}u+\frac{y}{\sqrt{x^2+y^2}}v \\ \frac{-y}{x^2+y^2}u+\frac{x}{x^2+y^2}v \end{pmatrix}[/math]


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

Specific tangent

Take [ilmath]y=x+1[/ilmath], at [ilmath]x=1[/ilmath] we see [ilmath]\frac{dy}{dx}=1[/ilmath], that is to say the tangent at [ilmath]p=(1,2)[/ilmath] is [ilmath](1,1)_p[/ilmath]

[math]\text{Jac}(\beta\circ\alpha^{-1})\begin{pmatrix} 1 \\ 1 \end{pmatrix} = \begin{pmatrix} \frac{3\sqrt{5}}{5} \\ \frac{-1}{5} \end{pmatrix}[/math] (using graphical calculator)

From this we see:

[math]\frac{dr}{d\theta}=\frac{\frac{3\sqrt{5}}{5}}{\frac{-1}{5}}=-3\sqrt{5}\approx-6.708\text{ (4sf)}[/math]


Using my graphical calculator I found:

[math]\left.\frac{d}{dt}\left[ |c|\sqrt{\frac{(m^2+1)}{(\tan(t)-m)^2}+\frac{2m}{\tan(t)-m}+1} \right]\right|_{t=\arctan(\frac{y}{x})}\approx -6.708\text{ (4sf)}[/math]
where
  • [ilmath]m=1[/ilmath]
  • [ilmath]c=1[/ilmath]
  • [ilmath](x,y)=p[/ilmath]



TODO: get back to tangent space



References

  1. Polar equation of a line