Finite subgroups of motoins always fix some point on the plane.












0












$begingroup$




Let $G$ be a finite subgroup of the group of motoins $M$ on the plane. Then there exists a point on the plane which is left fixed by every element of $G$.





The proof of this is sketched by our instructor as follows $:$



Let $s$ be an element on the plane. Let $S$ be the set of all images of $s$ under the action of the elements of $G$ on $s$. Then every element of $G$ permutes the elements of $S$. To see this let us take $f in G,s' in S$. If we can show that $f(s') in S$ then we are through. Since $s' in S$ $exists$ $g in G$ such that $g(s) = s'$. Since $f,g in G$ so $fg in G$. Therefore $fg (s) in G$ i.e. $f(s') in S,$ as claimed. Since $G$ is finite, $S$ is also finite. Let $S = {s_1,s_2, cdots , s_n }.$



After that our instructor asserted that the element $s^{*} = frac {1} {n} (s_1 + s_2 + cdots + s_n)$ is fixed by every element of $G$. This is the stage where I am struggling. Why $s^{*}$ is fixed by every element of $G$? If the element is rotation about origin or reflection about a line passing through origin then I have understood that the claim is true because they are linear operators which act linearly on $s^{*}$ and permute the $s_i$'s. Since vector addition is commutative we get $s^{*}$ back by acting them on $s^{*}$. Also clearly $G$ doesn't contain any proper translation since they are of infinite order. So what are the elements of $G$ other than rotations about origin and translations about a line through origin? I know that the elements of the group of motoins $M$ are either of the form $t_{a} rho_{theta}$ (which are precisely rotations about some point fixed by it ) or of the form $t_{a} rho_{theta}r$ (which are precisely glide reflections). So according to me the elements of $G$ is either of the form $t_{a} rho_{theta}$ or of the form $rho_{theta} r$. Do they all fix $s^{*}$? Please help me in this regard.



Thank you very much.










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$endgroup$












  • $begingroup$
    I have proved it on my own at least. Thank you very much.
    $endgroup$
    – Dbchatto67
    Dec 24 '18 at 16:01










  • $begingroup$
    I have proved that any rigid transformations take center of gravity to the center of gravity.
    $endgroup$
    – Dbchatto67
    Dec 24 '18 at 16:03












  • $begingroup$
    To be explicit let $m in M$ and let $S={s_1,s_2, cdots , s_n }$ be any finite collection of points on the plane. Let $s = frac {1} {n} (s_1+ s_2 + cdots + s_n)$ then $m(s) = s'$ where $s' = frac {1} {n} (m(s_1) + m(s_2) + cdots + m(s_n))$.
    $endgroup$
    – Dbchatto67
    Dec 24 '18 at 16:09










  • $begingroup$
    In this case $m in G$ and it permutes the elements of $S$. Since vector addition is commutative so we have $s'=s$, as claimed.
    $endgroup$
    – Dbchatto67
    Dec 24 '18 at 16:11


















0












$begingroup$




Let $G$ be a finite subgroup of the group of motoins $M$ on the plane. Then there exists a point on the plane which is left fixed by every element of $G$.





The proof of this is sketched by our instructor as follows $:$



Let $s$ be an element on the plane. Let $S$ be the set of all images of $s$ under the action of the elements of $G$ on $s$. Then every element of $G$ permutes the elements of $S$. To see this let us take $f in G,s' in S$. If we can show that $f(s') in S$ then we are through. Since $s' in S$ $exists$ $g in G$ such that $g(s) = s'$. Since $f,g in G$ so $fg in G$. Therefore $fg (s) in G$ i.e. $f(s') in S,$ as claimed. Since $G$ is finite, $S$ is also finite. Let $S = {s_1,s_2, cdots , s_n }.$



After that our instructor asserted that the element $s^{*} = frac {1} {n} (s_1 + s_2 + cdots + s_n)$ is fixed by every element of $G$. This is the stage where I am struggling. Why $s^{*}$ is fixed by every element of $G$? If the element is rotation about origin or reflection about a line passing through origin then I have understood that the claim is true because they are linear operators which act linearly on $s^{*}$ and permute the $s_i$'s. Since vector addition is commutative we get $s^{*}$ back by acting them on $s^{*}$. Also clearly $G$ doesn't contain any proper translation since they are of infinite order. So what are the elements of $G$ other than rotations about origin and translations about a line through origin? I know that the elements of the group of motoins $M$ are either of the form $t_{a} rho_{theta}$ (which are precisely rotations about some point fixed by it ) or of the form $t_{a} rho_{theta}r$ (which are precisely glide reflections). So according to me the elements of $G$ is either of the form $t_{a} rho_{theta}$ or of the form $rho_{theta} r$. Do they all fix $s^{*}$? Please help me in this regard.



Thank you very much.










share|cite|improve this question











$endgroup$












  • $begingroup$
    I have proved it on my own at least. Thank you very much.
    $endgroup$
    – Dbchatto67
    Dec 24 '18 at 16:01










  • $begingroup$
    I have proved that any rigid transformations take center of gravity to the center of gravity.
    $endgroup$
    – Dbchatto67
    Dec 24 '18 at 16:03












  • $begingroup$
    To be explicit let $m in M$ and let $S={s_1,s_2, cdots , s_n }$ be any finite collection of points on the plane. Let $s = frac {1} {n} (s_1+ s_2 + cdots + s_n)$ then $m(s) = s'$ where $s' = frac {1} {n} (m(s_1) + m(s_2) + cdots + m(s_n))$.
    $endgroup$
    – Dbchatto67
    Dec 24 '18 at 16:09










  • $begingroup$
    In this case $m in G$ and it permutes the elements of $S$. Since vector addition is commutative so we have $s'=s$, as claimed.
    $endgroup$
    – Dbchatto67
    Dec 24 '18 at 16:11
















0












0








0





$begingroup$




Let $G$ be a finite subgroup of the group of motoins $M$ on the plane. Then there exists a point on the plane which is left fixed by every element of $G$.





The proof of this is sketched by our instructor as follows $:$



Let $s$ be an element on the plane. Let $S$ be the set of all images of $s$ under the action of the elements of $G$ on $s$. Then every element of $G$ permutes the elements of $S$. To see this let us take $f in G,s' in S$. If we can show that $f(s') in S$ then we are through. Since $s' in S$ $exists$ $g in G$ such that $g(s) = s'$. Since $f,g in G$ so $fg in G$. Therefore $fg (s) in G$ i.e. $f(s') in S,$ as claimed. Since $G$ is finite, $S$ is also finite. Let $S = {s_1,s_2, cdots , s_n }.$



After that our instructor asserted that the element $s^{*} = frac {1} {n} (s_1 + s_2 + cdots + s_n)$ is fixed by every element of $G$. This is the stage where I am struggling. Why $s^{*}$ is fixed by every element of $G$? If the element is rotation about origin or reflection about a line passing through origin then I have understood that the claim is true because they are linear operators which act linearly on $s^{*}$ and permute the $s_i$'s. Since vector addition is commutative we get $s^{*}$ back by acting them on $s^{*}$. Also clearly $G$ doesn't contain any proper translation since they are of infinite order. So what are the elements of $G$ other than rotations about origin and translations about a line through origin? I know that the elements of the group of motoins $M$ are either of the form $t_{a} rho_{theta}$ (which are precisely rotations about some point fixed by it ) or of the form $t_{a} rho_{theta}r$ (which are precisely glide reflections). So according to me the elements of $G$ is either of the form $t_{a} rho_{theta}$ or of the form $rho_{theta} r$. Do they all fix $s^{*}$? Please help me in this regard.



Thank you very much.










share|cite|improve this question











$endgroup$






Let $G$ be a finite subgroup of the group of motoins $M$ on the plane. Then there exists a point on the plane which is left fixed by every element of $G$.





The proof of this is sketched by our instructor as follows $:$



Let $s$ be an element on the plane. Let $S$ be the set of all images of $s$ under the action of the elements of $G$ on $s$. Then every element of $G$ permutes the elements of $S$. To see this let us take $f in G,s' in S$. If we can show that $f(s') in S$ then we are through. Since $s' in S$ $exists$ $g in G$ such that $g(s) = s'$. Since $f,g in G$ so $fg in G$. Therefore $fg (s) in G$ i.e. $f(s') in S,$ as claimed. Since $G$ is finite, $S$ is also finite. Let $S = {s_1,s_2, cdots , s_n }.$



After that our instructor asserted that the element $s^{*} = frac {1} {n} (s_1 + s_2 + cdots + s_n)$ is fixed by every element of $G$. This is the stage where I am struggling. Why $s^{*}$ is fixed by every element of $G$? If the element is rotation about origin or reflection about a line passing through origin then I have understood that the claim is true because they are linear operators which act linearly on $s^{*}$ and permute the $s_i$'s. Since vector addition is commutative we get $s^{*}$ back by acting them on $s^{*}$. Also clearly $G$ doesn't contain any proper translation since they are of infinite order. So what are the elements of $G$ other than rotations about origin and translations about a line through origin? I know that the elements of the group of motoins $M$ are either of the form $t_{a} rho_{theta}$ (which are precisely rotations about some point fixed by it ) or of the form $t_{a} rho_{theta}r$ (which are precisely glide reflections). So according to me the elements of $G$ is either of the form $t_{a} rho_{theta}$ or of the form $rho_{theta} r$. Do they all fix $s^{*}$? Please help me in this regard.



Thank you very much.







abstract-algebra rigid-transformation






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share|cite|improve this question













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share|cite|improve this question








edited Dec 24 '18 at 15:42







Dbchatto67

















asked Dec 24 '18 at 15:38









Dbchatto67Dbchatto67

1,629219




1,629219












  • $begingroup$
    I have proved it on my own at least. Thank you very much.
    $endgroup$
    – Dbchatto67
    Dec 24 '18 at 16:01










  • $begingroup$
    I have proved that any rigid transformations take center of gravity to the center of gravity.
    $endgroup$
    – Dbchatto67
    Dec 24 '18 at 16:03












  • $begingroup$
    To be explicit let $m in M$ and let $S={s_1,s_2, cdots , s_n }$ be any finite collection of points on the plane. Let $s = frac {1} {n} (s_1+ s_2 + cdots + s_n)$ then $m(s) = s'$ where $s' = frac {1} {n} (m(s_1) + m(s_2) + cdots + m(s_n))$.
    $endgroup$
    – Dbchatto67
    Dec 24 '18 at 16:09










  • $begingroup$
    In this case $m in G$ and it permutes the elements of $S$. Since vector addition is commutative so we have $s'=s$, as claimed.
    $endgroup$
    – Dbchatto67
    Dec 24 '18 at 16:11




















  • $begingroup$
    I have proved it on my own at least. Thank you very much.
    $endgroup$
    – Dbchatto67
    Dec 24 '18 at 16:01










  • $begingroup$
    I have proved that any rigid transformations take center of gravity to the center of gravity.
    $endgroup$
    – Dbchatto67
    Dec 24 '18 at 16:03












  • $begingroup$
    To be explicit let $m in M$ and let $S={s_1,s_2, cdots , s_n }$ be any finite collection of points on the plane. Let $s = frac {1} {n} (s_1+ s_2 + cdots + s_n)$ then $m(s) = s'$ where $s' = frac {1} {n} (m(s_1) + m(s_2) + cdots + m(s_n))$.
    $endgroup$
    – Dbchatto67
    Dec 24 '18 at 16:09










  • $begingroup$
    In this case $m in G$ and it permutes the elements of $S$. Since vector addition is commutative so we have $s'=s$, as claimed.
    $endgroup$
    – Dbchatto67
    Dec 24 '18 at 16:11


















$begingroup$
I have proved it on my own at least. Thank you very much.
$endgroup$
– Dbchatto67
Dec 24 '18 at 16:01




$begingroup$
I have proved it on my own at least. Thank you very much.
$endgroup$
– Dbchatto67
Dec 24 '18 at 16:01












$begingroup$
I have proved that any rigid transformations take center of gravity to the center of gravity.
$endgroup$
– Dbchatto67
Dec 24 '18 at 16:03






$begingroup$
I have proved that any rigid transformations take center of gravity to the center of gravity.
$endgroup$
– Dbchatto67
Dec 24 '18 at 16:03














$begingroup$
To be explicit let $m in M$ and let $S={s_1,s_2, cdots , s_n }$ be any finite collection of points on the plane. Let $s = frac {1} {n} (s_1+ s_2 + cdots + s_n)$ then $m(s) = s'$ where $s' = frac {1} {n} (m(s_1) + m(s_2) + cdots + m(s_n))$.
$endgroup$
– Dbchatto67
Dec 24 '18 at 16:09




$begingroup$
To be explicit let $m in M$ and let $S={s_1,s_2, cdots , s_n }$ be any finite collection of points on the plane. Let $s = frac {1} {n} (s_1+ s_2 + cdots + s_n)$ then $m(s) = s'$ where $s' = frac {1} {n} (m(s_1) + m(s_2) + cdots + m(s_n))$.
$endgroup$
– Dbchatto67
Dec 24 '18 at 16:09












$begingroup$
In this case $m in G$ and it permutes the elements of $S$. Since vector addition is commutative so we have $s'=s$, as claimed.
$endgroup$
– Dbchatto67
Dec 24 '18 at 16:11






$begingroup$
In this case $m in G$ and it permutes the elements of $S$. Since vector addition is commutative so we have $s'=s$, as claimed.
$endgroup$
– Dbchatto67
Dec 24 '18 at 16:11












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