What is an improper affine space at infinity? Schouten: Tensor Analysis for Physicists
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Edit to add: This clearly deals with projective geometry. If I figure it out well enough to post a satisfactory answer, I will do so. If someone else posts a decent answer before then, I will be happy to give you the brownie points.
This question pertains to Tensor Analysis for Physicists, Second Edition, By: J. A. Schouten.
My understanding of what has been said leading to the quoted statement is as follows:
A space of all allowable coordinate systems under the affine group of $mathbbR^n$ is called an affine space, or an $E_n$. The space of all allowable coordinate system under the centered affine group of $mathbbR^n$ is called a centered $E_n$.
The space of all allowable coordinate systems resulting from centered affine transformations of the solution set of the system of $n-p$ linearly independent equations
$$C_nu^ix^nu+C^i=0,$$
is called a flat sub-manifold of $E_n$, and is an $E_p$. Two $E_p$'s are said to be parallel if they can be transformed into each other by a translation. Two parallel $E_p$'s are said to have the same $p-textdirection.$
After introducing the concept of the intersection of $E_p$'s and $E_q$'s, Schouten states:
[W]e consider the points of $E_p$ 'at infinity' as an improper $E_p-1$ (or $E_p-1$ at infinity. Then two parallel $E_p-1$'s intersect in an improper $E_p-1,$ and from this we see that an improper $E_p-1$ may be considered as a $p-textdirection.$
That statement makes very little sense to me. Can this be stated in terms of a traditional Euclidean 2-plane in 3-space, in a way that clarifies Schouten's statement? Am I to envision translating the plane parallel to itself to "positive infinity"? Am I to consider the "boundary" of the plane at the infinite extremes of its coordinate axes?
The statement appears following equation 3.9 on page 5. It is available in the preview.
linear-algebra group-theory linear-transformations tensors projective-geometry
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up vote
1
down vote
favorite
Edit to add: This clearly deals with projective geometry. If I figure it out well enough to post a satisfactory answer, I will do so. If someone else posts a decent answer before then, I will be happy to give you the brownie points.
This question pertains to Tensor Analysis for Physicists, Second Edition, By: J. A. Schouten.
My understanding of what has been said leading to the quoted statement is as follows:
A space of all allowable coordinate systems under the affine group of $mathbbR^n$ is called an affine space, or an $E_n$. The space of all allowable coordinate system under the centered affine group of $mathbbR^n$ is called a centered $E_n$.
The space of all allowable coordinate systems resulting from centered affine transformations of the solution set of the system of $n-p$ linearly independent equations
$$C_nu^ix^nu+C^i=0,$$
is called a flat sub-manifold of $E_n$, and is an $E_p$. Two $E_p$'s are said to be parallel if they can be transformed into each other by a translation. Two parallel $E_p$'s are said to have the same $p-textdirection.$
After introducing the concept of the intersection of $E_p$'s and $E_q$'s, Schouten states:
[W]e consider the points of $E_p$ 'at infinity' as an improper $E_p-1$ (or $E_p-1$ at infinity. Then two parallel $E_p-1$'s intersect in an improper $E_p-1,$ and from this we see that an improper $E_p-1$ may be considered as a $p-textdirection.$
That statement makes very little sense to me. Can this be stated in terms of a traditional Euclidean 2-plane in 3-space, in a way that clarifies Schouten's statement? Am I to envision translating the plane parallel to itself to "positive infinity"? Am I to consider the "boundary" of the plane at the infinite extremes of its coordinate axes?
The statement appears following equation 3.9 on page 5. It is available in the preview.
linear-algebra group-theory linear-transformations tensors projective-geometry
add a comment |Â
up vote
1
down vote
favorite
up vote
1
down vote
favorite
Edit to add: This clearly deals with projective geometry. If I figure it out well enough to post a satisfactory answer, I will do so. If someone else posts a decent answer before then, I will be happy to give you the brownie points.
This question pertains to Tensor Analysis for Physicists, Second Edition, By: J. A. Schouten.
My understanding of what has been said leading to the quoted statement is as follows:
A space of all allowable coordinate systems under the affine group of $mathbbR^n$ is called an affine space, or an $E_n$. The space of all allowable coordinate system under the centered affine group of $mathbbR^n$ is called a centered $E_n$.
The space of all allowable coordinate systems resulting from centered affine transformations of the solution set of the system of $n-p$ linearly independent equations
$$C_nu^ix^nu+C^i=0,$$
is called a flat sub-manifold of $E_n$, and is an $E_p$. Two $E_p$'s are said to be parallel if they can be transformed into each other by a translation. Two parallel $E_p$'s are said to have the same $p-textdirection.$
After introducing the concept of the intersection of $E_p$'s and $E_q$'s, Schouten states:
[W]e consider the points of $E_p$ 'at infinity' as an improper $E_p-1$ (or $E_p-1$ at infinity. Then two parallel $E_p-1$'s intersect in an improper $E_p-1,$ and from this we see that an improper $E_p-1$ may be considered as a $p-textdirection.$
That statement makes very little sense to me. Can this be stated in terms of a traditional Euclidean 2-plane in 3-space, in a way that clarifies Schouten's statement? Am I to envision translating the plane parallel to itself to "positive infinity"? Am I to consider the "boundary" of the plane at the infinite extremes of its coordinate axes?
The statement appears following equation 3.9 on page 5. It is available in the preview.
linear-algebra group-theory linear-transformations tensors projective-geometry
Edit to add: This clearly deals with projective geometry. If I figure it out well enough to post a satisfactory answer, I will do so. If someone else posts a decent answer before then, I will be happy to give you the brownie points.
This question pertains to Tensor Analysis for Physicists, Second Edition, By: J. A. Schouten.
My understanding of what has been said leading to the quoted statement is as follows:
A space of all allowable coordinate systems under the affine group of $mathbbR^n$ is called an affine space, or an $E_n$. The space of all allowable coordinate system under the centered affine group of $mathbbR^n$ is called a centered $E_n$.
The space of all allowable coordinate systems resulting from centered affine transformations of the solution set of the system of $n-p$ linearly independent equations
$$C_nu^ix^nu+C^i=0,$$
is called a flat sub-manifold of $E_n$, and is an $E_p$. Two $E_p$'s are said to be parallel if they can be transformed into each other by a translation. Two parallel $E_p$'s are said to have the same $p-textdirection.$
After introducing the concept of the intersection of $E_p$'s and $E_q$'s, Schouten states:
[W]e consider the points of $E_p$ 'at infinity' as an improper $E_p-1$ (or $E_p-1$ at infinity. Then two parallel $E_p-1$'s intersect in an improper $E_p-1,$ and from this we see that an improper $E_p-1$ may be considered as a $p-textdirection.$
That statement makes very little sense to me. Can this be stated in terms of a traditional Euclidean 2-plane in 3-space, in a way that clarifies Schouten's statement? Am I to envision translating the plane parallel to itself to "positive infinity"? Am I to consider the "boundary" of the plane at the infinite extremes of its coordinate axes?
The statement appears following equation 3.9 on page 5. It is available in the preview.
linear-algebra group-theory linear-transformations tensors projective-geometry
edited Aug 17 at 21:05
asked Aug 17 at 7:40
Steven Hatton
672314
672314
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