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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 $f$?
$begingroup$
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.
calculus multivariable-calculus differential-geometry vector-spaces taylor-expansion
$endgroup$
add a comment |
$begingroup$
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.
calculus multivariable-calculus differential-geometry vector-spaces taylor-expansion
$endgroup$
add a comment |
$begingroup$
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.
calculus multivariable-calculus differential-geometry vector-spaces taylor-expansion
$endgroup$
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
calculus multivariable-calculus differential-geometry vector-spaces taylor-expansion
edited Mar 29 at 15:03
Takeshi Gouda
asked Mar 29 at 13:54
Takeshi GoudaTakeshi Gouda
264
264
add a comment |
add a comment |
1 Answer
1
active
oldest
votes
$begingroup$
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.
$endgroup$
$begingroup$
This makes so much more sense! Thank you!
$endgroup$
– Takeshi Gouda
Mar 30 at 12:39
add a comment |
Your Answer
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1 Answer
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1 Answer
1
active
oldest
votes
active
oldest
votes
active
oldest
votes
$begingroup$
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.
$endgroup$
$begingroup$
This makes so much more sense! Thank you!
$endgroup$
– Takeshi Gouda
Mar 30 at 12:39
add a comment |
$begingroup$
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.
$endgroup$
$begingroup$
This makes so much more sense! Thank you!
$endgroup$
– Takeshi Gouda
Mar 30 at 12:39
add a comment |
$begingroup$
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.
$endgroup$
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.
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
add a comment |
$begingroup$
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
add a comment |
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