vector field of real projective space
$begingroup$
Let $RP^n$ the real projective space. This is a manifold and i have take the usual charts in order to prove it. The problem is that i don't know how to define a vector field on that.
Since $RP^n$ is a set of lines that passes through the point (0,...,0) could I claim that the vector space is a map that takes every point of $RP^n$ - line and sends it to a vector $overline {OP}$ ,where O is the origin and P is a point of the line ?
Is there a concrete example on $PR^2$?
manifolds
$endgroup$
add a comment |
$begingroup$
Let $RP^n$ the real projective space. This is a manifold and i have take the usual charts in order to prove it. The problem is that i don't know how to define a vector field on that.
Since $RP^n$ is a set of lines that passes through the point (0,...,0) could I claim that the vector space is a map that takes every point of $RP^n$ - line and sends it to a vector $overline {OP}$ ,where O is the origin and P is a point of the line ?
Is there a concrete example on $PR^2$?
manifolds
$endgroup$
add a comment |
$begingroup$
Let $RP^n$ the real projective space. This is a manifold and i have take the usual charts in order to prove it. The problem is that i don't know how to define a vector field on that.
Since $RP^n$ is a set of lines that passes through the point (0,...,0) could I claim that the vector space is a map that takes every point of $RP^n$ - line and sends it to a vector $overline {OP}$ ,where O is the origin and P is a point of the line ?
Is there a concrete example on $PR^2$?
manifolds
$endgroup$
Let $RP^n$ the real projective space. This is a manifold and i have take the usual charts in order to prove it. The problem is that i don't know how to define a vector field on that.
Since $RP^n$ is a set of lines that passes through the point (0,...,0) could I claim that the vector space is a map that takes every point of $RP^n$ - line and sends it to a vector $overline {OP}$ ,where O is the origin and P is a point of the line ?
Is there a concrete example on $PR^2$?
manifolds
manifolds
asked Jan 27 at 15:48
janejane
264
264
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1 Answer
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$begingroup$
We can visualize $RP^2$ as the plane in $mathbb R^3$ at $z=1$.
We can write a point as $(x:y:1)$. Or more generally as $(x:y:z)$, which we consider equivalent to $(frac xz:frac yz:1)$ if $zne 0$. Consequently all points on a line through the origin are equivalent. And a point $(x:y:0)$ is a point at infinity, which is also an element of $RP^2$.
An obvious choice for a local chart is $phi: (x:y:1)mapsto (x,y)$.
Taking the partial derivatives gives us the representations $fracpartial{partial x}=(1:0:0)$ and $fracpartial{partial y}=(0:1:0)$. Note that these correspond exactly with the standard unit vectors in the plane $z=1$.
A vector field $X: RP^2to TRP^2$ can now locally be written as:
$$X(mathbf x) = X(x:y:1) = xi(mathbf x)fracpartial{partial x} + eta(mathbf x)fracpartial{partial y} = (xi(mathbf x):eta(mathbf x):0)$$
$endgroup$
1
$begingroup$
oh...i get it ..thanks...
$endgroup$
– jane
Feb 3 at 17:33
add a comment |
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1 Answer
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1 Answer
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$begingroup$
We can visualize $RP^2$ as the plane in $mathbb R^3$ at $z=1$.
We can write a point as $(x:y:1)$. Or more generally as $(x:y:z)$, which we consider equivalent to $(frac xz:frac yz:1)$ if $zne 0$. Consequently all points on a line through the origin are equivalent. And a point $(x:y:0)$ is a point at infinity, which is also an element of $RP^2$.
An obvious choice for a local chart is $phi: (x:y:1)mapsto (x,y)$.
Taking the partial derivatives gives us the representations $fracpartial{partial x}=(1:0:0)$ and $fracpartial{partial y}=(0:1:0)$. Note that these correspond exactly with the standard unit vectors in the plane $z=1$.
A vector field $X: RP^2to TRP^2$ can now locally be written as:
$$X(mathbf x) = X(x:y:1) = xi(mathbf x)fracpartial{partial x} + eta(mathbf x)fracpartial{partial y} = (xi(mathbf x):eta(mathbf x):0)$$
$endgroup$
1
$begingroup$
oh...i get it ..thanks...
$endgroup$
– jane
Feb 3 at 17:33
add a comment |
$begingroup$
We can visualize $RP^2$ as the plane in $mathbb R^3$ at $z=1$.
We can write a point as $(x:y:1)$. Or more generally as $(x:y:z)$, which we consider equivalent to $(frac xz:frac yz:1)$ if $zne 0$. Consequently all points on a line through the origin are equivalent. And a point $(x:y:0)$ is a point at infinity, which is also an element of $RP^2$.
An obvious choice for a local chart is $phi: (x:y:1)mapsto (x,y)$.
Taking the partial derivatives gives us the representations $fracpartial{partial x}=(1:0:0)$ and $fracpartial{partial y}=(0:1:0)$. Note that these correspond exactly with the standard unit vectors in the plane $z=1$.
A vector field $X: RP^2to TRP^2$ can now locally be written as:
$$X(mathbf x) = X(x:y:1) = xi(mathbf x)fracpartial{partial x} + eta(mathbf x)fracpartial{partial y} = (xi(mathbf x):eta(mathbf x):0)$$
$endgroup$
1
$begingroup$
oh...i get it ..thanks...
$endgroup$
– jane
Feb 3 at 17:33
add a comment |
$begingroup$
We can visualize $RP^2$ as the plane in $mathbb R^3$ at $z=1$.
We can write a point as $(x:y:1)$. Or more generally as $(x:y:z)$, which we consider equivalent to $(frac xz:frac yz:1)$ if $zne 0$. Consequently all points on a line through the origin are equivalent. And a point $(x:y:0)$ is a point at infinity, which is also an element of $RP^2$.
An obvious choice for a local chart is $phi: (x:y:1)mapsto (x,y)$.
Taking the partial derivatives gives us the representations $fracpartial{partial x}=(1:0:0)$ and $fracpartial{partial y}=(0:1:0)$. Note that these correspond exactly with the standard unit vectors in the plane $z=1$.
A vector field $X: RP^2to TRP^2$ can now locally be written as:
$$X(mathbf x) = X(x:y:1) = xi(mathbf x)fracpartial{partial x} + eta(mathbf x)fracpartial{partial y} = (xi(mathbf x):eta(mathbf x):0)$$
$endgroup$
We can visualize $RP^2$ as the plane in $mathbb R^3$ at $z=1$.
We can write a point as $(x:y:1)$. Or more generally as $(x:y:z)$, which we consider equivalent to $(frac xz:frac yz:1)$ if $zne 0$. Consequently all points on a line through the origin are equivalent. And a point $(x:y:0)$ is a point at infinity, which is also an element of $RP^2$.
An obvious choice for a local chart is $phi: (x:y:1)mapsto (x,y)$.
Taking the partial derivatives gives us the representations $fracpartial{partial x}=(1:0:0)$ and $fracpartial{partial y}=(0:1:0)$. Note that these correspond exactly with the standard unit vectors in the plane $z=1$.
A vector field $X: RP^2to TRP^2$ can now locally be written as:
$$X(mathbf x) = X(x:y:1) = xi(mathbf x)fracpartial{partial x} + eta(mathbf x)fracpartial{partial y} = (xi(mathbf x):eta(mathbf x):0)$$
answered Feb 2 at 20:18
Klaas van AarsenKlaas van Aarsen
4,3421822
4,3421822
1
$begingroup$
oh...i get it ..thanks...
$endgroup$
– jane
Feb 3 at 17:33
add a comment |
1
$begingroup$
oh...i get it ..thanks...
$endgroup$
– jane
Feb 3 at 17:33
1
1
$begingroup$
oh...i get it ..thanks...
$endgroup$
– jane
Feb 3 at 17:33
$begingroup$
oh...i get it ..thanks...
$endgroup$
– jane
Feb 3 at 17:33
add a comment |
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