Isometry of $mathbb R^2$ that preserves orientation is either a rotation or a translation
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I want to show that if $gamma$ is an isometry of $mathbb{R}^2$ that preserves orientation, then it is either a translation or a rotation about a point.
If $gamma$ is an isometry of $mathbb{R}^2$ then it is of the form $vec{gamma}(vec{x})=Avec{x}+vec{b}$ for some orthogonal matrix $A$ and $vec{b} in mathbb{R}^2$. Since $gamma$ preserves orientation we have that $det A=1$.
If $A=I$, then clearly $gamma$ is a translation $vec{x} mapsto vec{x} + vec{b}$.
I'm stuck with the case $A neq I$, though. How do I proceed?
geometry geometric-transformation
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add a comment |
$begingroup$
I want to show that if $gamma$ is an isometry of $mathbb{R}^2$ that preserves orientation, then it is either a translation or a rotation about a point.
If $gamma$ is an isometry of $mathbb{R}^2$ then it is of the form $vec{gamma}(vec{x})=Avec{x}+vec{b}$ for some orthogonal matrix $A$ and $vec{b} in mathbb{R}^2$. Since $gamma$ preserves orientation we have that $det A=1$.
If $A=I$, then clearly $gamma$ is a translation $vec{x} mapsto vec{x} + vec{b}$.
I'm stuck with the case $A neq I$, though. How do I proceed?
geometry geometric-transformation
$endgroup$
add a comment |
$begingroup$
I want to show that if $gamma$ is an isometry of $mathbb{R}^2$ that preserves orientation, then it is either a translation or a rotation about a point.
If $gamma$ is an isometry of $mathbb{R}^2$ then it is of the form $vec{gamma}(vec{x})=Avec{x}+vec{b}$ for some orthogonal matrix $A$ and $vec{b} in mathbb{R}^2$. Since $gamma$ preserves orientation we have that $det A=1$.
If $A=I$, then clearly $gamma$ is a translation $vec{x} mapsto vec{x} + vec{b}$.
I'm stuck with the case $A neq I$, though. How do I proceed?
geometry geometric-transformation
$endgroup$
I want to show that if $gamma$ is an isometry of $mathbb{R}^2$ that preserves orientation, then it is either a translation or a rotation about a point.
If $gamma$ is an isometry of $mathbb{R}^2$ then it is of the form $vec{gamma}(vec{x})=Avec{x}+vec{b}$ for some orthogonal matrix $A$ and $vec{b} in mathbb{R}^2$. Since $gamma$ preserves orientation we have that $det A=1$.
If $A=I$, then clearly $gamma$ is a translation $vec{x} mapsto vec{x} + vec{b}$.
I'm stuck with the case $A neq I$, though. How do I proceed?
geometry geometric-transformation
geometry geometric-transformation
edited Jan 28 at 19:28
greedoid
46.1k1160117
46.1k1160117
asked Feb 14 '17 at 20:14
Si.0788Si.0788
1,302627
1,302627
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2 Answers
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Orthogonal matrices with determinant 1 are exactly rotation matrices (about the origin). Hence $vec{gamma}(vec{x})=Avec{x}+vec{b}$ is a rotation plus a translation, i.e. a rotation about the point which has the coordinates of the vector $vec{b}$.
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1
$begingroup$
It's rather a rotation that takes $0$ into $b$.
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– Berci
Feb 14 '17 at 20:27
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How would one justify that a rotation plus a translation is indeed a rotation about the point $vec{b}$?
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– Si.0788
Feb 15 '17 at 17:20
add a comment |
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First observe that translations are rigid motoins or isometry and any rigid motion which fixes the origin preserves the inner product i.e. any rigid motion which fixes the origin is an orthogonal transformation. Now suppose $m$ is an isometry. Then $m$ sends the origin $O$ to somewhere let's say $b$ i.e. $m(O) = b,$ where $b in Bbb R^n$. Let $t_{-b}$ be the translation by the vector $-b$ i.e. $t_{-b} (v) = v-b, v in Bbb R^n$. Let $A=t_{-b} circ m$. Then clearly $A$ is an isometry since so are $t_{-b}$ and $v$. Also $A(O) = O$ i.e. $A$ fixes the origin. So by our previous observation it follows that $A$ is an orthogonal transformation. Since translations are invertible and $t_{-b} = (t_b)^{-1}$ for all $b in Bbb R^n$. So we have $m = t_b circ A$. So $m(v) = Av + b, text {for all} v in Bbb R^n$ where $A in O(n)$.
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2 Answers
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active
oldest
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2 Answers
2
active
oldest
votes
active
oldest
votes
active
oldest
votes
$begingroup$
Orthogonal matrices with determinant 1 are exactly rotation matrices (about the origin). Hence $vec{gamma}(vec{x})=Avec{x}+vec{b}$ is a rotation plus a translation, i.e. a rotation about the point which has the coordinates of the vector $vec{b}$.
$endgroup$
1
$begingroup$
It's rather a rotation that takes $0$ into $b$.
$endgroup$
– Berci
Feb 14 '17 at 20:27
$begingroup$
How would one justify that a rotation plus a translation is indeed a rotation about the point $vec{b}$?
$endgroup$
– Si.0788
Feb 15 '17 at 17:20
add a comment |
$begingroup$
Orthogonal matrices with determinant 1 are exactly rotation matrices (about the origin). Hence $vec{gamma}(vec{x})=Avec{x}+vec{b}$ is a rotation plus a translation, i.e. a rotation about the point which has the coordinates of the vector $vec{b}$.
$endgroup$
1
$begingroup$
It's rather a rotation that takes $0$ into $b$.
$endgroup$
– Berci
Feb 14 '17 at 20:27
$begingroup$
How would one justify that a rotation plus a translation is indeed a rotation about the point $vec{b}$?
$endgroup$
– Si.0788
Feb 15 '17 at 17:20
add a comment |
$begingroup$
Orthogonal matrices with determinant 1 are exactly rotation matrices (about the origin). Hence $vec{gamma}(vec{x})=Avec{x}+vec{b}$ is a rotation plus a translation, i.e. a rotation about the point which has the coordinates of the vector $vec{b}$.
$endgroup$
Orthogonal matrices with determinant 1 are exactly rotation matrices (about the origin). Hence $vec{gamma}(vec{x})=Avec{x}+vec{b}$ is a rotation plus a translation, i.e. a rotation about the point which has the coordinates of the vector $vec{b}$.
answered Feb 14 '17 at 20:25
MuziMuzi
424320
424320
1
$begingroup$
It's rather a rotation that takes $0$ into $b$.
$endgroup$
– Berci
Feb 14 '17 at 20:27
$begingroup$
How would one justify that a rotation plus a translation is indeed a rotation about the point $vec{b}$?
$endgroup$
– Si.0788
Feb 15 '17 at 17:20
add a comment |
1
$begingroup$
It's rather a rotation that takes $0$ into $b$.
$endgroup$
– Berci
Feb 14 '17 at 20:27
$begingroup$
How would one justify that a rotation plus a translation is indeed a rotation about the point $vec{b}$?
$endgroup$
– Si.0788
Feb 15 '17 at 17:20
1
1
$begingroup$
It's rather a rotation that takes $0$ into $b$.
$endgroup$
– Berci
Feb 14 '17 at 20:27
$begingroup$
It's rather a rotation that takes $0$ into $b$.
$endgroup$
– Berci
Feb 14 '17 at 20:27
$begingroup$
How would one justify that a rotation plus a translation is indeed a rotation about the point $vec{b}$?
$endgroup$
– Si.0788
Feb 15 '17 at 17:20
$begingroup$
How would one justify that a rotation plus a translation is indeed a rotation about the point $vec{b}$?
$endgroup$
– Si.0788
Feb 15 '17 at 17:20
add a comment |
$begingroup$
First observe that translations are rigid motoins or isometry and any rigid motion which fixes the origin preserves the inner product i.e. any rigid motion which fixes the origin is an orthogonal transformation. Now suppose $m$ is an isometry. Then $m$ sends the origin $O$ to somewhere let's say $b$ i.e. $m(O) = b,$ where $b in Bbb R^n$. Let $t_{-b}$ be the translation by the vector $-b$ i.e. $t_{-b} (v) = v-b, v in Bbb R^n$. Let $A=t_{-b} circ m$. Then clearly $A$ is an isometry since so are $t_{-b}$ and $v$. Also $A(O) = O$ i.e. $A$ fixes the origin. So by our previous observation it follows that $A$ is an orthogonal transformation. Since translations are invertible and $t_{-b} = (t_b)^{-1}$ for all $b in Bbb R^n$. So we have $m = t_b circ A$. So $m(v) = Av + b, text {for all} v in Bbb R^n$ where $A in O(n)$.
$endgroup$
add a comment |
$begingroup$
First observe that translations are rigid motoins or isometry and any rigid motion which fixes the origin preserves the inner product i.e. any rigid motion which fixes the origin is an orthogonal transformation. Now suppose $m$ is an isometry. Then $m$ sends the origin $O$ to somewhere let's say $b$ i.e. $m(O) = b,$ where $b in Bbb R^n$. Let $t_{-b}$ be the translation by the vector $-b$ i.e. $t_{-b} (v) = v-b, v in Bbb R^n$. Let $A=t_{-b} circ m$. Then clearly $A$ is an isometry since so are $t_{-b}$ and $v$. Also $A(O) = O$ i.e. $A$ fixes the origin. So by our previous observation it follows that $A$ is an orthogonal transformation. Since translations are invertible and $t_{-b} = (t_b)^{-1}$ for all $b in Bbb R^n$. So we have $m = t_b circ A$. So $m(v) = Av + b, text {for all} v in Bbb R^n$ where $A in O(n)$.
$endgroup$
add a comment |
$begingroup$
First observe that translations are rigid motoins or isometry and any rigid motion which fixes the origin preserves the inner product i.e. any rigid motion which fixes the origin is an orthogonal transformation. Now suppose $m$ is an isometry. Then $m$ sends the origin $O$ to somewhere let's say $b$ i.e. $m(O) = b,$ where $b in Bbb R^n$. Let $t_{-b}$ be the translation by the vector $-b$ i.e. $t_{-b} (v) = v-b, v in Bbb R^n$. Let $A=t_{-b} circ m$. Then clearly $A$ is an isometry since so are $t_{-b}$ and $v$. Also $A(O) = O$ i.e. $A$ fixes the origin. So by our previous observation it follows that $A$ is an orthogonal transformation. Since translations are invertible and $t_{-b} = (t_b)^{-1}$ for all $b in Bbb R^n$. So we have $m = t_b circ A$. So $m(v) = Av + b, text {for all} v in Bbb R^n$ where $A in O(n)$.
$endgroup$
First observe that translations are rigid motoins or isometry and any rigid motion which fixes the origin preserves the inner product i.e. any rigid motion which fixes the origin is an orthogonal transformation. Now suppose $m$ is an isometry. Then $m$ sends the origin $O$ to somewhere let's say $b$ i.e. $m(O) = b,$ where $b in Bbb R^n$. Let $t_{-b}$ be the translation by the vector $-b$ i.e. $t_{-b} (v) = v-b, v in Bbb R^n$. Let $A=t_{-b} circ m$. Then clearly $A$ is an isometry since so are $t_{-b}$ and $v$. Also $A(O) = O$ i.e. $A$ fixes the origin. So by our previous observation it follows that $A$ is an orthogonal transformation. Since translations are invertible and $t_{-b} = (t_b)^{-1}$ for all $b in Bbb R^n$. So we have $m = t_b circ A$. So $m(v) = Av + b, text {for all} v in Bbb R^n$ where $A in O(n)$.
edited Jan 28 at 19:18
answered Dec 22 '18 at 5:56
Dbchatto67Dbchatto67
1,631219
1,631219
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