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Basic question regarding Taylor series and local charts


Taylor series expansion and Laplace transform final value theoremA question on smooth functions and the Taylor seriesTaylor expansion of second orderMultivariable Taylor SeriesShow $df(fracpartialpartial x_jBig|_m ) = sum_i fracpartial(y_icirc f)partial x_j fracpartialpartial y_iBig|_f(m)$Convergence of Taylor series for smooth complex functionsDerivation of forward/backward/central difference methods from taylor seriesNewton-like multivariate, vector-valued root findingLinear function on space of smooth functions, Taylor seriesAt a Critical Point the Hessian Equals the Frst Nonconstant Term in the Taylor Series of $f$?













1












$begingroup$


I am reading a proof of a basic result in differential geometry, which I am having trouble following.



The statement is the following: Suppose $X$ is a vector field on $M$, a $C^infty$ manifold, and $(U; x_1, ..., x_n)$ be a coordinate chart. Then $X|_U$ can be uniquely expressed as
$$
X|_U = sum_j=1^n a_j fracpartialpartial x_j
$$

where $a_j in C^infty(M)$.



Proof presented goes as follows: Define $a_j = X x_j.$ Let $ f in C^infty(U)$ and $p in U$. Then we may write
$$
f = f(p) + sum_i fracpartial fpartial x_i (p) (x_i - x_i(p)) + h,
$$

where $h$ is a linear combination of products $h_1h_2$ with $h_1(p) = h_2(p) = 0$.
Then since $X$ is a derivation
$$
X(h_1 h_2)(p) = h_1(p) X h_2(p) + h_2(p) Xh_1(p) =0.
$$

From which point the statement is easy enough to deduce.



My question is: We only know $f$ is in $C^infty(U)$. How does one deduce about $h$ only from this information? I am having difficulty following this because $f$ may not have a converging Taylor series in which case I don't see how one can deduce that $h$ is a linear combination of products $h_1h_2$ with $h_1(p) = h_2(p) = 0$ (I can see this if we assume $f$ has a Taylor series expansion everywhere... but not sure how to see this here).



Thank you.










share|cite|improve this question











$endgroup$
















    1












    $begingroup$


    I am reading a proof of a basic result in differential geometry, which I am having trouble following.



    The statement is the following: Suppose $X$ is a vector field on $M$, a $C^infty$ manifold, and $(U; x_1, ..., x_n)$ be a coordinate chart. Then $X|_U$ can be uniquely expressed as
    $$
    X|_U = sum_j=1^n a_j fracpartialpartial x_j
    $$

    where $a_j in C^infty(M)$.



    Proof presented goes as follows: Define $a_j = X x_j.$ Let $ f in C^infty(U)$ and $p in U$. Then we may write
    $$
    f = f(p) + sum_i fracpartial fpartial x_i (p) (x_i - x_i(p)) + h,
    $$

    where $h$ is a linear combination of products $h_1h_2$ with $h_1(p) = h_2(p) = 0$.
    Then since $X$ is a derivation
    $$
    X(h_1 h_2)(p) = h_1(p) X h_2(p) + h_2(p) Xh_1(p) =0.
    $$

    From which point the statement is easy enough to deduce.



    My question is: We only know $f$ is in $C^infty(U)$. How does one deduce about $h$ only from this information? I am having difficulty following this because $f$ may not have a converging Taylor series in which case I don't see how one can deduce that $h$ is a linear combination of products $h_1h_2$ with $h_1(p) = h_2(p) = 0$ (I can see this if we assume $f$ has a Taylor series expansion everywhere... but not sure how to see this here).



    Thank you.










    share|cite|improve this question











    $endgroup$














      1












      1








      1





      $begingroup$


      I am reading a proof of a basic result in differential geometry, which I am having trouble following.



      The statement is the following: Suppose $X$ is a vector field on $M$, a $C^infty$ manifold, and $(U; x_1, ..., x_n)$ be a coordinate chart. Then $X|_U$ can be uniquely expressed as
      $$
      X|_U = sum_j=1^n a_j fracpartialpartial x_j
      $$

      where $a_j in C^infty(M)$.



      Proof presented goes as follows: Define $a_j = X x_j.$ Let $ f in C^infty(U)$ and $p in U$. Then we may write
      $$
      f = f(p) + sum_i fracpartial fpartial x_i (p) (x_i - x_i(p)) + h,
      $$

      where $h$ is a linear combination of products $h_1h_2$ with $h_1(p) = h_2(p) = 0$.
      Then since $X$ is a derivation
      $$
      X(h_1 h_2)(p) = h_1(p) X h_2(p) + h_2(p) Xh_1(p) =0.
      $$

      From which point the statement is easy enough to deduce.



      My question is: We only know $f$ is in $C^infty(U)$. How does one deduce about $h$ only from this information? I am having difficulty following this because $f$ may not have a converging Taylor series in which case I don't see how one can deduce that $h$ is a linear combination of products $h_1h_2$ with $h_1(p) = h_2(p) = 0$ (I can see this if we assume $f$ has a Taylor series expansion everywhere... but not sure how to see this here).



      Thank you.










      share|cite|improve this question











      $endgroup$




      I am reading a proof of a basic result in differential geometry, which I am having trouble following.



      The statement is the following: Suppose $X$ is a vector field on $M$, a $C^infty$ manifold, and $(U; x_1, ..., x_n)$ be a coordinate chart. Then $X|_U$ can be uniquely expressed as
      $$
      X|_U = sum_j=1^n a_j fracpartialpartial x_j
      $$

      where $a_j in C^infty(M)$.



      Proof presented goes as follows: Define $a_j = X x_j.$ Let $ f in C^infty(U)$ and $p in U$. Then we may write
      $$
      f = f(p) + sum_i fracpartial fpartial x_i (p) (x_i - x_i(p)) + h,
      $$

      where $h$ is a linear combination of products $h_1h_2$ with $h_1(p) = h_2(p) = 0$.
      Then since $X$ is a derivation
      $$
      X(h_1 h_2)(p) = h_1(p) X h_2(p) + h_2(p) Xh_1(p) =0.
      $$

      From which point the statement is easy enough to deduce.



      My question is: We only know $f$ is in $C^infty(U)$. How does one deduce about $h$ only from this information? I am having difficulty following this because $f$ may not have a converging Taylor series in which case I don't see how one can deduce that $h$ is a linear combination of products $h_1h_2$ with $h_1(p) = h_2(p) = 0$ (I can see this if we assume $f$ has a Taylor series expansion everywhere... but not sure how to see this here).



      Thank you.







      calculus multivariable-calculus differential-geometry vector-spaces taylor-expansion






      share|cite|improve this question















      share|cite|improve this question













      share|cite|improve this question




      share|cite|improve this question








      edited Mar 29 at 15:03







      Takeshi Gouda

















      asked Mar 29 at 13:54









      Takeshi GoudaTakeshi Gouda

      264




      264




















          1 Answer
          1






          active

          oldest

          votes


















          0












          $begingroup$

          The standard proof is to write
          $$f(x)=f(p) + sum g_i(x)(x_i-x_i(p))$$
          where $g_i$ is smooth and $g_i(p) = partial f/partial x_i(p)$. Working in $Bbb R^n$ with $p=0$, just write
          $$f(x) = f(0) + int_0^1 frac ddt f(tx),dt$$
          and use the chain rule.






          share|cite|improve this answer









          $endgroup$












          • $begingroup$
            This makes so much more sense! Thank you!
            $endgroup$
            – Takeshi Gouda
            Mar 30 at 12:39











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          1 Answer
          1






          active

          oldest

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          active

          oldest

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          active

          oldest

          votes









          0












          $begingroup$

          The standard proof is to write
          $$f(x)=f(p) + sum g_i(x)(x_i-x_i(p))$$
          where $g_i$ is smooth and $g_i(p) = partial f/partial x_i(p)$. Working in $Bbb R^n$ with $p=0$, just write
          $$f(x) = f(0) + int_0^1 frac ddt f(tx),dt$$
          and use the chain rule.






          share|cite|improve this answer









          $endgroup$












          • $begingroup$
            This makes so much more sense! Thank you!
            $endgroup$
            – Takeshi Gouda
            Mar 30 at 12:39















          0












          $begingroup$

          The standard proof is to write
          $$f(x)=f(p) + sum g_i(x)(x_i-x_i(p))$$
          where $g_i$ is smooth and $g_i(p) = partial f/partial x_i(p)$. Working in $Bbb R^n$ with $p=0$, just write
          $$f(x) = f(0) + int_0^1 frac ddt f(tx),dt$$
          and use the chain rule.






          share|cite|improve this answer









          $endgroup$












          • $begingroup$
            This makes so much more sense! Thank you!
            $endgroup$
            – Takeshi Gouda
            Mar 30 at 12:39













          0












          0








          0





          $begingroup$

          The standard proof is to write
          $$f(x)=f(p) + sum g_i(x)(x_i-x_i(p))$$
          where $g_i$ is smooth and $g_i(p) = partial f/partial x_i(p)$. Working in $Bbb R^n$ with $p=0$, just write
          $$f(x) = f(0) + int_0^1 frac ddt f(tx),dt$$
          and use the chain rule.






          share|cite|improve this answer









          $endgroup$



          The standard proof is to write
          $$f(x)=f(p) + sum g_i(x)(x_i-x_i(p))$$
          where $g_i$ is smooth and $g_i(p) = partial f/partial x_i(p)$. Working in $Bbb R^n$ with $p=0$, just write
          $$f(x) = f(0) + int_0^1 frac ddt f(tx),dt$$
          and use the chain rule.







          share|cite|improve this answer












          share|cite|improve this answer



          share|cite|improve this answer










          answered Mar 29 at 16:13









          Ted ShifrinTed Shifrin

          64.8k44692




          64.8k44692











          • $begingroup$
            This makes so much more sense! Thank you!
            $endgroup$
            – Takeshi Gouda
            Mar 30 at 12:39
















          • $begingroup$
            This makes so much more sense! Thank you!
            $endgroup$
            – Takeshi Gouda
            Mar 30 at 12:39















          $begingroup$
          This makes so much more sense! Thank you!
          $endgroup$
          – Takeshi Gouda
          Mar 30 at 12:39




          $begingroup$
          This makes so much more sense! Thank you!
          $endgroup$
          – Takeshi Gouda
          Mar 30 at 12:39

















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