How do I compose isometries algebraically?

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I've learned the general gist of isometries: reflections, translations, rotations, and glide reflections.



However, I've been taught this geometrically. So when I want to find what $textref_l(textref_m)$ (composition of two reflections at different lines $m$ and $l$) is for example, I can only draw certain shape like a triangle and see that it can be a rotation. However, apparently it can also be a translation (no idea how).



I'm asking if there are rules that can algebraically help me determine that and similar things like:



(a) a reflection in some line $l$ followed by a rotation about a point on $l$, (b) rotation about a point followed by a rotation about a different point. Are there algebraic rules of composition that can help me determine what type of isometries that these can represent?







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  • You assume isometries of the plane $BbbR^2$? We can use matrices.
    – Dietrich Burde
    Aug 3 at 20:55











  • @DietrichBurde Yes, sorry I should have said that. It's all in $mathbbR^2$. I'd love to know this matrices method.
    – Nebulae
    Aug 3 at 20:57















up vote
0
down vote

favorite












I've learned the general gist of isometries: reflections, translations, rotations, and glide reflections.



However, I've been taught this geometrically. So when I want to find what $textref_l(textref_m)$ (composition of two reflections at different lines $m$ and $l$) is for example, I can only draw certain shape like a triangle and see that it can be a rotation. However, apparently it can also be a translation (no idea how).



I'm asking if there are rules that can algebraically help me determine that and similar things like:



(a) a reflection in some line $l$ followed by a rotation about a point on $l$, (b) rotation about a point followed by a rotation about a different point. Are there algebraic rules of composition that can help me determine what type of isometries that these can represent?







share|cite|improve this question



















  • You assume isometries of the plane $BbbR^2$? We can use matrices.
    – Dietrich Burde
    Aug 3 at 20:55











  • @DietrichBurde Yes, sorry I should have said that. It's all in $mathbbR^2$. I'd love to know this matrices method.
    – Nebulae
    Aug 3 at 20:57













up vote
0
down vote

favorite









up vote
0
down vote

favorite











I've learned the general gist of isometries: reflections, translations, rotations, and glide reflections.



However, I've been taught this geometrically. So when I want to find what $textref_l(textref_m)$ (composition of two reflections at different lines $m$ and $l$) is for example, I can only draw certain shape like a triangle and see that it can be a rotation. However, apparently it can also be a translation (no idea how).



I'm asking if there are rules that can algebraically help me determine that and similar things like:



(a) a reflection in some line $l$ followed by a rotation about a point on $l$, (b) rotation about a point followed by a rotation about a different point. Are there algebraic rules of composition that can help me determine what type of isometries that these can represent?







share|cite|improve this question











I've learned the general gist of isometries: reflections, translations, rotations, and glide reflections.



However, I've been taught this geometrically. So when I want to find what $textref_l(textref_m)$ (composition of two reflections at different lines $m$ and $l$) is for example, I can only draw certain shape like a triangle and see that it can be a rotation. However, apparently it can also be a translation (no idea how).



I'm asking if there are rules that can algebraically help me determine that and similar things like:



(a) a reflection in some line $l$ followed by a rotation about a point on $l$, (b) rotation about a point followed by a rotation about a different point. Are there algebraic rules of composition that can help me determine what type of isometries that these can represent?









share|cite|improve this question










share|cite|improve this question




share|cite|improve this question









asked Aug 3 at 20:44









Nebulae

435




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  • You assume isometries of the plane $BbbR^2$? We can use matrices.
    – Dietrich Burde
    Aug 3 at 20:55











  • @DietrichBurde Yes, sorry I should have said that. It's all in $mathbbR^2$. I'd love to know this matrices method.
    – Nebulae
    Aug 3 at 20:57

















  • You assume isometries of the plane $BbbR^2$? We can use matrices.
    – Dietrich Burde
    Aug 3 at 20:55











  • @DietrichBurde Yes, sorry I should have said that. It's all in $mathbbR^2$. I'd love to know this matrices method.
    – Nebulae
    Aug 3 at 20:57
















You assume isometries of the plane $BbbR^2$? We can use matrices.
– Dietrich Burde
Aug 3 at 20:55





You assume isometries of the plane $BbbR^2$? We can use matrices.
– Dietrich Burde
Aug 3 at 20:55













@DietrichBurde Yes, sorry I should have said that. It's all in $mathbbR^2$. I'd love to know this matrices method.
– Nebulae
Aug 3 at 20:57





@DietrichBurde Yes, sorry I should have said that. It's all in $mathbbR^2$. I'd love to know this matrices method.
– Nebulae
Aug 3 at 20:57











2 Answers
2






active

oldest

votes

















up vote
2
down vote



accepted










The orientation perserving isometry group of the plane is $SO_2(mathbbR)rtimesmathbbR^2$ (the orthogonal group $SO_2(mathbbR)$ are the rotations and $mathbbR^2$ are the translations). This can be embedded in $SL_3(mathbbR)$ as follows:
$$
left(
beginarrayccc
1&0&0\
a&costheta&-sintheta\
b&sintheta&costheta\
endarray
right) textfirst rotation by theta text then translation by (a,b).
$$
This acts on a point $(x,y)$ of the plane by
$$
left(
beginarrayccc
1&0&0\
a&costheta&-sintheta\
b&sintheta&costheta\
endarray
right)
left(
beginarrayc
1\
x\
y\
endarray
right).
$$
For instance if $theta=0$ we get the translation
$$
(x,y)mapsto(a+x,b+y)
$$
or if $a=b=0$ we get the rotation
$$
(x,y)mapsto(xcostheta+ysintheta,xsintheta-ycostheta).
$$
Together we get a rotation by $theta$ followed by a translation by $(a,b)$:
$$
(x,y)mapsto(a+xcostheta+ysintheta,b+xsintheta-ycostheta).
$$
This also extends as you might think to the full isometry group $O_2(mathbbR)rtimesmathbbR^2$ by throwing in a reflection, e.g.
$$
left(
beginarrayccc
1&0&0\
0&-1&0\
0&0&1\
endarray
right), (x,y)mapsto(-x,y),
$$
and it also extends to higher dimension in the obvious way.






share|cite|improve this answer





















  • Thank you very much for this. Regarding the reflection matrix M, does it act on the $(x,y)$ by plane via $M (1,x,y)^t$? where $t$ denotes the transpose, like the rotation-translation matrix you've given? So If I want to find translation(rotation(reflection)), what would it look like? I may need to read more about this, and this will be clarified. I appreciate your work, though, this is massively helpful!
    – Nebulae
    Aug 3 at 22:50

















up vote
0
down vote













Yes, those formulas exist. The reflection of a point $(p,q)$ on the line $ax+by+c=0$ is$$left(fracp(a^2-b^2)-2b(aq+c)a^2+b^2,fracq(b^2-a^2)-2a(bp+c)a^2+b^2right).$$The rotation of $(p,q)$ with angle $theta$ around $(a,b)$ is$$bigl(a+(p-a)cos(theta )-(q-b)sin(theta),b+(p-a) sin (theta )+(q-b) cos (theta )bigr).$$You can use these formulas to compute the composition of rotations or of reflections.






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    2 Answers
    2






    active

    oldest

    votes








    2 Answers
    2






    active

    oldest

    votes









    active

    oldest

    votes






    active

    oldest

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    up vote
    2
    down vote



    accepted










    The orientation perserving isometry group of the plane is $SO_2(mathbbR)rtimesmathbbR^2$ (the orthogonal group $SO_2(mathbbR)$ are the rotations and $mathbbR^2$ are the translations). This can be embedded in $SL_3(mathbbR)$ as follows:
    $$
    left(
    beginarrayccc
    1&0&0\
    a&costheta&-sintheta\
    b&sintheta&costheta\
    endarray
    right) textfirst rotation by theta text then translation by (a,b).
    $$
    This acts on a point $(x,y)$ of the plane by
    $$
    left(
    beginarrayccc
    1&0&0\
    a&costheta&-sintheta\
    b&sintheta&costheta\
    endarray
    right)
    left(
    beginarrayc
    1\
    x\
    y\
    endarray
    right).
    $$
    For instance if $theta=0$ we get the translation
    $$
    (x,y)mapsto(a+x,b+y)
    $$
    or if $a=b=0$ we get the rotation
    $$
    (x,y)mapsto(xcostheta+ysintheta,xsintheta-ycostheta).
    $$
    Together we get a rotation by $theta$ followed by a translation by $(a,b)$:
    $$
    (x,y)mapsto(a+xcostheta+ysintheta,b+xsintheta-ycostheta).
    $$
    This also extends as you might think to the full isometry group $O_2(mathbbR)rtimesmathbbR^2$ by throwing in a reflection, e.g.
    $$
    left(
    beginarrayccc
    1&0&0\
    0&-1&0\
    0&0&1\
    endarray
    right), (x,y)mapsto(-x,y),
    $$
    and it also extends to higher dimension in the obvious way.






    share|cite|improve this answer





















    • Thank you very much for this. Regarding the reflection matrix M, does it act on the $(x,y)$ by plane via $M (1,x,y)^t$? where $t$ denotes the transpose, like the rotation-translation matrix you've given? So If I want to find translation(rotation(reflection)), what would it look like? I may need to read more about this, and this will be clarified. I appreciate your work, though, this is massively helpful!
      – Nebulae
      Aug 3 at 22:50














    up vote
    2
    down vote



    accepted










    The orientation perserving isometry group of the plane is $SO_2(mathbbR)rtimesmathbbR^2$ (the orthogonal group $SO_2(mathbbR)$ are the rotations and $mathbbR^2$ are the translations). This can be embedded in $SL_3(mathbbR)$ as follows:
    $$
    left(
    beginarrayccc
    1&0&0\
    a&costheta&-sintheta\
    b&sintheta&costheta\
    endarray
    right) textfirst rotation by theta text then translation by (a,b).
    $$
    This acts on a point $(x,y)$ of the plane by
    $$
    left(
    beginarrayccc
    1&0&0\
    a&costheta&-sintheta\
    b&sintheta&costheta\
    endarray
    right)
    left(
    beginarrayc
    1\
    x\
    y\
    endarray
    right).
    $$
    For instance if $theta=0$ we get the translation
    $$
    (x,y)mapsto(a+x,b+y)
    $$
    or if $a=b=0$ we get the rotation
    $$
    (x,y)mapsto(xcostheta+ysintheta,xsintheta-ycostheta).
    $$
    Together we get a rotation by $theta$ followed by a translation by $(a,b)$:
    $$
    (x,y)mapsto(a+xcostheta+ysintheta,b+xsintheta-ycostheta).
    $$
    This also extends as you might think to the full isometry group $O_2(mathbbR)rtimesmathbbR^2$ by throwing in a reflection, e.g.
    $$
    left(
    beginarrayccc
    1&0&0\
    0&-1&0\
    0&0&1\
    endarray
    right), (x,y)mapsto(-x,y),
    $$
    and it also extends to higher dimension in the obvious way.






    share|cite|improve this answer





















    • Thank you very much for this. Regarding the reflection matrix M, does it act on the $(x,y)$ by plane via $M (1,x,y)^t$? where $t$ denotes the transpose, like the rotation-translation matrix you've given? So If I want to find translation(rotation(reflection)), what would it look like? I may need to read more about this, and this will be clarified. I appreciate your work, though, this is massively helpful!
      – Nebulae
      Aug 3 at 22:50












    up vote
    2
    down vote



    accepted







    up vote
    2
    down vote



    accepted






    The orientation perserving isometry group of the plane is $SO_2(mathbbR)rtimesmathbbR^2$ (the orthogonal group $SO_2(mathbbR)$ are the rotations and $mathbbR^2$ are the translations). This can be embedded in $SL_3(mathbbR)$ as follows:
    $$
    left(
    beginarrayccc
    1&0&0\
    a&costheta&-sintheta\
    b&sintheta&costheta\
    endarray
    right) textfirst rotation by theta text then translation by (a,b).
    $$
    This acts on a point $(x,y)$ of the plane by
    $$
    left(
    beginarrayccc
    1&0&0\
    a&costheta&-sintheta\
    b&sintheta&costheta\
    endarray
    right)
    left(
    beginarrayc
    1\
    x\
    y\
    endarray
    right).
    $$
    For instance if $theta=0$ we get the translation
    $$
    (x,y)mapsto(a+x,b+y)
    $$
    or if $a=b=0$ we get the rotation
    $$
    (x,y)mapsto(xcostheta+ysintheta,xsintheta-ycostheta).
    $$
    Together we get a rotation by $theta$ followed by a translation by $(a,b)$:
    $$
    (x,y)mapsto(a+xcostheta+ysintheta,b+xsintheta-ycostheta).
    $$
    This also extends as you might think to the full isometry group $O_2(mathbbR)rtimesmathbbR^2$ by throwing in a reflection, e.g.
    $$
    left(
    beginarrayccc
    1&0&0\
    0&-1&0\
    0&0&1\
    endarray
    right), (x,y)mapsto(-x,y),
    $$
    and it also extends to higher dimension in the obvious way.






    share|cite|improve this answer













    The orientation perserving isometry group of the plane is $SO_2(mathbbR)rtimesmathbbR^2$ (the orthogonal group $SO_2(mathbbR)$ are the rotations and $mathbbR^2$ are the translations). This can be embedded in $SL_3(mathbbR)$ as follows:
    $$
    left(
    beginarrayccc
    1&0&0\
    a&costheta&-sintheta\
    b&sintheta&costheta\
    endarray
    right) textfirst rotation by theta text then translation by (a,b).
    $$
    This acts on a point $(x,y)$ of the plane by
    $$
    left(
    beginarrayccc
    1&0&0\
    a&costheta&-sintheta\
    b&sintheta&costheta\
    endarray
    right)
    left(
    beginarrayc
    1\
    x\
    y\
    endarray
    right).
    $$
    For instance if $theta=0$ we get the translation
    $$
    (x,y)mapsto(a+x,b+y)
    $$
    or if $a=b=0$ we get the rotation
    $$
    (x,y)mapsto(xcostheta+ysintheta,xsintheta-ycostheta).
    $$
    Together we get a rotation by $theta$ followed by a translation by $(a,b)$:
    $$
    (x,y)mapsto(a+xcostheta+ysintheta,b+xsintheta-ycostheta).
    $$
    This also extends as you might think to the full isometry group $O_2(mathbbR)rtimesmathbbR^2$ by throwing in a reflection, e.g.
    $$
    left(
    beginarrayccc
    1&0&0\
    0&-1&0\
    0&0&1\
    endarray
    right), (x,y)mapsto(-x,y),
    $$
    and it also extends to higher dimension in the obvious way.







    share|cite|improve this answer













    share|cite|improve this answer



    share|cite|improve this answer











    answered Aug 3 at 21:42









    yoyo

    6,3291525




    6,3291525











    • Thank you very much for this. Regarding the reflection matrix M, does it act on the $(x,y)$ by plane via $M (1,x,y)^t$? where $t$ denotes the transpose, like the rotation-translation matrix you've given? So If I want to find translation(rotation(reflection)), what would it look like? I may need to read more about this, and this will be clarified. I appreciate your work, though, this is massively helpful!
      – Nebulae
      Aug 3 at 22:50
















    • Thank you very much for this. Regarding the reflection matrix M, does it act on the $(x,y)$ by plane via $M (1,x,y)^t$? where $t$ denotes the transpose, like the rotation-translation matrix you've given? So If I want to find translation(rotation(reflection)), what would it look like? I may need to read more about this, and this will be clarified. I appreciate your work, though, this is massively helpful!
      – Nebulae
      Aug 3 at 22:50















    Thank you very much for this. Regarding the reflection matrix M, does it act on the $(x,y)$ by plane via $M (1,x,y)^t$? where $t$ denotes the transpose, like the rotation-translation matrix you've given? So If I want to find translation(rotation(reflection)), what would it look like? I may need to read more about this, and this will be clarified. I appreciate your work, though, this is massively helpful!
    – Nebulae
    Aug 3 at 22:50




    Thank you very much for this. Regarding the reflection matrix M, does it act on the $(x,y)$ by plane via $M (1,x,y)^t$? where $t$ denotes the transpose, like the rotation-translation matrix you've given? So If I want to find translation(rotation(reflection)), what would it look like? I may need to read more about this, and this will be clarified. I appreciate your work, though, this is massively helpful!
    – Nebulae
    Aug 3 at 22:50










    up vote
    0
    down vote













    Yes, those formulas exist. The reflection of a point $(p,q)$ on the line $ax+by+c=0$ is$$left(fracp(a^2-b^2)-2b(aq+c)a^2+b^2,fracq(b^2-a^2)-2a(bp+c)a^2+b^2right).$$The rotation of $(p,q)$ with angle $theta$ around $(a,b)$ is$$bigl(a+(p-a)cos(theta )-(q-b)sin(theta),b+(p-a) sin (theta )+(q-b) cos (theta )bigr).$$You can use these formulas to compute the composition of rotations or of reflections.






    share|cite|improve this answer

























      up vote
      0
      down vote













      Yes, those formulas exist. The reflection of a point $(p,q)$ on the line $ax+by+c=0$ is$$left(fracp(a^2-b^2)-2b(aq+c)a^2+b^2,fracq(b^2-a^2)-2a(bp+c)a^2+b^2right).$$The rotation of $(p,q)$ with angle $theta$ around $(a,b)$ is$$bigl(a+(p-a)cos(theta )-(q-b)sin(theta),b+(p-a) sin (theta )+(q-b) cos (theta )bigr).$$You can use these formulas to compute the composition of rotations or of reflections.






      share|cite|improve this answer























        up vote
        0
        down vote










        up vote
        0
        down vote









        Yes, those formulas exist. The reflection of a point $(p,q)$ on the line $ax+by+c=0$ is$$left(fracp(a^2-b^2)-2b(aq+c)a^2+b^2,fracq(b^2-a^2)-2a(bp+c)a^2+b^2right).$$The rotation of $(p,q)$ with angle $theta$ around $(a,b)$ is$$bigl(a+(p-a)cos(theta )-(q-b)sin(theta),b+(p-a) sin (theta )+(q-b) cos (theta )bigr).$$You can use these formulas to compute the composition of rotations or of reflections.






        share|cite|improve this answer













        Yes, those formulas exist. The reflection of a point $(p,q)$ on the line $ax+by+c=0$ is$$left(fracp(a^2-b^2)-2b(aq+c)a^2+b^2,fracq(b^2-a^2)-2a(bp+c)a^2+b^2right).$$The rotation of $(p,q)$ with angle $theta$ around $(a,b)$ is$$bigl(a+(p-a)cos(theta )-(q-b)sin(theta),b+(p-a) sin (theta )+(q-b) cos (theta )bigr).$$You can use these formulas to compute the composition of rotations or of reflections.







        share|cite|improve this answer













        share|cite|improve this answer



        share|cite|improve this answer











        answered Aug 3 at 21:09









        José Carlos Santos

        112k1696172




        112k1696172






















             

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