(Updates on this title are welcome..) Function-valued functions in differential equations

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I'm trying to prove the problem below:



Let $Omega = (omega_ij)$ be a skew-symmetric $3×3$ matrix, i.e., $Omega^T=-Omega$.



Let $e_1(s)$, $e_2(s)$ and $e_3(s)$ be smooth vector-valued functions of a parametre $s$ satisfying the differential equations $fracddse_i=sum^3_k=1 omega_ik e_k$, where $i=1,2,3$.



Suppose that for some parametre value $s_0$, the vectors $e_1(s_0)$, $e_2(s_0)$ and $e_3(s_0)$ are orthonormal.



Show that the vectors $e_1(s)$, $e_2(s)$ and $e_3(s)$ are orthonormal for all $s$.



=



But what I have been doing is just expanding out the differential equations $fracddse_i$ and translating the condition of "orthonormal" for $e_1(s_0)$, $e_2(s_0)$ and $e_3(s_0)$.



I have also defined a function $f_ik(s)=e_i(s) cdot e_k(s)$, where $i,k=1,2,3$, and found its derivative by the product rule: $fracddsf_ik(s)=fracddse_i(s) cdot e_k(s) + e_i(s) cdot fracddse_k(s)$.



Any ideas on how to carrying on this proof? Thanks!







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  • If you want to learn more about similar equations, a fantastic resource is the book by Murray, Li and Sastry on "A Mathematical Introduction to Robotic Manipulation" cds.caltech.edu/~murray/books/MLS/pdf/mls94-complete.pdf
    – WalterJ
    Aug 6 at 23:35






  • 1




    Thanks heaps would look into it :)
    – Evelyn Venne
    Aug 7 at 2:19














up vote
0
down vote

favorite












I'm trying to prove the problem below:



Let $Omega = (omega_ij)$ be a skew-symmetric $3×3$ matrix, i.e., $Omega^T=-Omega$.



Let $e_1(s)$, $e_2(s)$ and $e_3(s)$ be smooth vector-valued functions of a parametre $s$ satisfying the differential equations $fracddse_i=sum^3_k=1 omega_ik e_k$, where $i=1,2,3$.



Suppose that for some parametre value $s_0$, the vectors $e_1(s_0)$, $e_2(s_0)$ and $e_3(s_0)$ are orthonormal.



Show that the vectors $e_1(s)$, $e_2(s)$ and $e_3(s)$ are orthonormal for all $s$.



=



But what I have been doing is just expanding out the differential equations $fracddse_i$ and translating the condition of "orthonormal" for $e_1(s_0)$, $e_2(s_0)$ and $e_3(s_0)$.



I have also defined a function $f_ik(s)=e_i(s) cdot e_k(s)$, where $i,k=1,2,3$, and found its derivative by the product rule: $fracddsf_ik(s)=fracddse_i(s) cdot e_k(s) + e_i(s) cdot fracddse_k(s)$.



Any ideas on how to carrying on this proof? Thanks!







share|cite|improve this question





















  • If you want to learn more about similar equations, a fantastic resource is the book by Murray, Li and Sastry on "A Mathematical Introduction to Robotic Manipulation" cds.caltech.edu/~murray/books/MLS/pdf/mls94-complete.pdf
    – WalterJ
    Aug 6 at 23:35






  • 1




    Thanks heaps would look into it :)
    – Evelyn Venne
    Aug 7 at 2:19












up vote
0
down vote

favorite









up vote
0
down vote

favorite











I'm trying to prove the problem below:



Let $Omega = (omega_ij)$ be a skew-symmetric $3×3$ matrix, i.e., $Omega^T=-Omega$.



Let $e_1(s)$, $e_2(s)$ and $e_3(s)$ be smooth vector-valued functions of a parametre $s$ satisfying the differential equations $fracddse_i=sum^3_k=1 omega_ik e_k$, where $i=1,2,3$.



Suppose that for some parametre value $s_0$, the vectors $e_1(s_0)$, $e_2(s_0)$ and $e_3(s_0)$ are orthonormal.



Show that the vectors $e_1(s)$, $e_2(s)$ and $e_3(s)$ are orthonormal for all $s$.



=



But what I have been doing is just expanding out the differential equations $fracddse_i$ and translating the condition of "orthonormal" for $e_1(s_0)$, $e_2(s_0)$ and $e_3(s_0)$.



I have also defined a function $f_ik(s)=e_i(s) cdot e_k(s)$, where $i,k=1,2,3$, and found its derivative by the product rule: $fracddsf_ik(s)=fracddse_i(s) cdot e_k(s) + e_i(s) cdot fracddse_k(s)$.



Any ideas on how to carrying on this proof? Thanks!







share|cite|improve this question













I'm trying to prove the problem below:



Let $Omega = (omega_ij)$ be a skew-symmetric $3×3$ matrix, i.e., $Omega^T=-Omega$.



Let $e_1(s)$, $e_2(s)$ and $e_3(s)$ be smooth vector-valued functions of a parametre $s$ satisfying the differential equations $fracddse_i=sum^3_k=1 omega_ik e_k$, where $i=1,2,3$.



Suppose that for some parametre value $s_0$, the vectors $e_1(s_0)$, $e_2(s_0)$ and $e_3(s_0)$ are orthonormal.



Show that the vectors $e_1(s)$, $e_2(s)$ and $e_3(s)$ are orthonormal for all $s$.



=



But what I have been doing is just expanding out the differential equations $fracddse_i$ and translating the condition of "orthonormal" for $e_1(s_0)$, $e_2(s_0)$ and $e_3(s_0)$.



I have also defined a function $f_ik(s)=e_i(s) cdot e_k(s)$, where $i,k=1,2,3$, and found its derivative by the product rule: $fracddsf_ik(s)=fracddse_i(s) cdot e_k(s) + e_i(s) cdot fracddse_k(s)$.



Any ideas on how to carrying on this proof? Thanks!









share|cite|improve this question












share|cite|improve this question




share|cite|improve this question








edited Aug 6 at 22:47
























asked Aug 6 at 22:32









Evelyn Venne

334




334











  • If you want to learn more about similar equations, a fantastic resource is the book by Murray, Li and Sastry on "A Mathematical Introduction to Robotic Manipulation" cds.caltech.edu/~murray/books/MLS/pdf/mls94-complete.pdf
    – WalterJ
    Aug 6 at 23:35






  • 1




    Thanks heaps would look into it :)
    – Evelyn Venne
    Aug 7 at 2:19
















  • If you want to learn more about similar equations, a fantastic resource is the book by Murray, Li and Sastry on "A Mathematical Introduction to Robotic Manipulation" cds.caltech.edu/~murray/books/MLS/pdf/mls94-complete.pdf
    – WalterJ
    Aug 6 at 23:35






  • 1




    Thanks heaps would look into it :)
    – Evelyn Venne
    Aug 7 at 2:19















If you want to learn more about similar equations, a fantastic resource is the book by Murray, Li and Sastry on "A Mathematical Introduction to Robotic Manipulation" cds.caltech.edu/~murray/books/MLS/pdf/mls94-complete.pdf
– WalterJ
Aug 6 at 23:35




If you want to learn more about similar equations, a fantastic resource is the book by Murray, Li and Sastry on "A Mathematical Introduction to Robotic Manipulation" cds.caltech.edu/~murray/books/MLS/pdf/mls94-complete.pdf
– WalterJ
Aug 6 at 23:35




1




1




Thanks heaps would look into it :)
– Evelyn Venne
Aug 7 at 2:19




Thanks heaps would look into it :)
– Evelyn Venne
Aug 7 at 2:19










1 Answer
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You can write the set of differential equations as
beginequation
fracpartialpartial sbeginpmatrix e_1(s) & e_2(s) & e_3(s) endpmatrix = Omega beginpmatrix e_1(s) & e_2(s) & e_3(s) endpmatrix
endequation
with the solution
beginalign
beginpmatrix e_1(s) & e_2(s) & e_3(s) endpmatrix &= e^Omega sbeginpmatrix e_1(s_0) & e_2(s_0) & e_3(s_0) endpmatrix\
&= e^-Omega^top sbeginpmatrix e_1(s_0) & e_2(s_0) & e_3(s_0) endpmatrix.
endalign
It turns out that $e^Omega s$ is a rotation matrix (formally you can look into the special orthogonal group), which means that for any $s$ the frame $beginpmatrix e_1(s_0) & e_2(s_0) & e_3(s_0) endpmatrix$ is rotated, which preserves relative orientation, e.g. pick up a box, you can rotate it all day long, the sides remain fixed with respect to each other.






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    1 Answer
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    1 Answer
    1






    active

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    active

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    active

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    up vote
    0
    down vote



    accepted










    You can write the set of differential equations as
    beginequation
    fracpartialpartial sbeginpmatrix e_1(s) & e_2(s) & e_3(s) endpmatrix = Omega beginpmatrix e_1(s) & e_2(s) & e_3(s) endpmatrix
    endequation
    with the solution
    beginalign
    beginpmatrix e_1(s) & e_2(s) & e_3(s) endpmatrix &= e^Omega sbeginpmatrix e_1(s_0) & e_2(s_0) & e_3(s_0) endpmatrix\
    &= e^-Omega^top sbeginpmatrix e_1(s_0) & e_2(s_0) & e_3(s_0) endpmatrix.
    endalign
    It turns out that $e^Omega s$ is a rotation matrix (formally you can look into the special orthogonal group), which means that for any $s$ the frame $beginpmatrix e_1(s_0) & e_2(s_0) & e_3(s_0) endpmatrix$ is rotated, which preserves relative orientation, e.g. pick up a box, you can rotate it all day long, the sides remain fixed with respect to each other.






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      up vote
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      down vote



      accepted










      You can write the set of differential equations as
      beginequation
      fracpartialpartial sbeginpmatrix e_1(s) & e_2(s) & e_3(s) endpmatrix = Omega beginpmatrix e_1(s) & e_2(s) & e_3(s) endpmatrix
      endequation
      with the solution
      beginalign
      beginpmatrix e_1(s) & e_2(s) & e_3(s) endpmatrix &= e^Omega sbeginpmatrix e_1(s_0) & e_2(s_0) & e_3(s_0) endpmatrix\
      &= e^-Omega^top sbeginpmatrix e_1(s_0) & e_2(s_0) & e_3(s_0) endpmatrix.
      endalign
      It turns out that $e^Omega s$ is a rotation matrix (formally you can look into the special orthogonal group), which means that for any $s$ the frame $beginpmatrix e_1(s_0) & e_2(s_0) & e_3(s_0) endpmatrix$ is rotated, which preserves relative orientation, e.g. pick up a box, you can rotate it all day long, the sides remain fixed with respect to each other.






      share|cite|improve this answer























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        down vote



        accepted







        up vote
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        You can write the set of differential equations as
        beginequation
        fracpartialpartial sbeginpmatrix e_1(s) & e_2(s) & e_3(s) endpmatrix = Omega beginpmatrix e_1(s) & e_2(s) & e_3(s) endpmatrix
        endequation
        with the solution
        beginalign
        beginpmatrix e_1(s) & e_2(s) & e_3(s) endpmatrix &= e^Omega sbeginpmatrix e_1(s_0) & e_2(s_0) & e_3(s_0) endpmatrix\
        &= e^-Omega^top sbeginpmatrix e_1(s_0) & e_2(s_0) & e_3(s_0) endpmatrix.
        endalign
        It turns out that $e^Omega s$ is a rotation matrix (formally you can look into the special orthogonal group), which means that for any $s$ the frame $beginpmatrix e_1(s_0) & e_2(s_0) & e_3(s_0) endpmatrix$ is rotated, which preserves relative orientation, e.g. pick up a box, you can rotate it all day long, the sides remain fixed with respect to each other.






        share|cite|improve this answer













        You can write the set of differential equations as
        beginequation
        fracpartialpartial sbeginpmatrix e_1(s) & e_2(s) & e_3(s) endpmatrix = Omega beginpmatrix e_1(s) & e_2(s) & e_3(s) endpmatrix
        endequation
        with the solution
        beginalign
        beginpmatrix e_1(s) & e_2(s) & e_3(s) endpmatrix &= e^Omega sbeginpmatrix e_1(s_0) & e_2(s_0) & e_3(s_0) endpmatrix\
        &= e^-Omega^top sbeginpmatrix e_1(s_0) & e_2(s_0) & e_3(s_0) endpmatrix.
        endalign
        It turns out that $e^Omega s$ is a rotation matrix (formally you can look into the special orthogonal group), which means that for any $s$ the frame $beginpmatrix e_1(s_0) & e_2(s_0) & e_3(s_0) endpmatrix$ is rotated, which preserves relative orientation, e.g. pick up a box, you can rotate it all day long, the sides remain fixed with respect to each other.







        share|cite|improve this answer













        share|cite|improve this answer



        share|cite|improve this answer











        answered Aug 6 at 23:25









        WalterJ

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