The part I think I understand. I'm mainly going through all this so that we know we're talking the same language, as I wasn't always sure what you meant by a "vector-valued function." A function whose range is a subset of [itex]\mathbb{R}^n[/itex], n > 1? A function whose range is either [itex]M[/itex] or a subset of [itex]\mathbb{R}^n[/itex], n > 1? (Some authors, in this context, make "vector" synonymous with tangent vector, an element of [itex]TM[/itex], the tangent bundle of the particular manifold under discussion; but then, a vector might simply mean a vector with respect to any vector space.) Also when you say "q(w) is a function" do you mean this literally, or should I read it as "q is a function"?
Background, definitions of notation and terminology:
[itex]M[/itex] is a smooth manifold. [itex]\gamma[/itex] is a curve, that is, a function of the from
[tex]\gamma : (a,b) \rightarrow M, \enspace\enspace a,b \in \overline{\mathbb{R}}.[/tex]
A tangent vector associated with point [itex]P \in M[/itex] is, according to the formalism Fecko is using in this section, an equivalence class of curves [itex][\gamma][/itex] such that for every pair of representatives [itex]\gamma[/itex] and [itex]\sigma[/itex], and every pair of charts [itex]x[/itex] and [itex]y[/itex], we have [itex]\gamma (t_0) = \sigma (t_0) = P[/itex], and
[tex]\frac{\mathrm{d} }{\mathrm{d} t} x \circ \gamma \bigg|_{t_0} = \frac{\mathrm{d} }{\mathrm{d} t} y \circ \sigma \bigg|_{t_0}.[/tex]
EDIT: Oops, not for every pair of charts, just for one chart.
The coordinate presentation of a curve, [itex]\gamma[/itex], in a chart [itex]x[/itex] is the function
[tex]x \circ \gamma : (a,b) \rightarrow \mathbb{R}^n,[/itex]<br />
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letting [itex]\circ[/itex] mean the function which makes any necessary restrictions to the range of [itex]\gamma[/itex] before composing it with [itex]x[/itex], in case the range of the curve contains elements outside of the domain of [itex]x[/itex].<br />
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A vector field is a function<br />
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[tex]V:M \rightarrow TM,[/itex]<br />
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i.e. one whose inputs are points in [itex]M[/itex] and whose outputs are tangent vectors.<br />
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Now, to the part I'm working on... Hmm, I see now that the third equation in my post #1 can't be right, since [itex]x^i : U \subseteq M \rightarrow \mathbb{R}[/itex], so the composition [itex]x^i \circ x^i[/itex] has range the empty set, if [itex]\circ[/itex] is taken to mean "restrict and compose", or is meaningless, if [itex]\circ[/itex] is taken to mean simply "compose".<br />
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While I'm pondering what you wrote, it might be useful to quote Fecko in full.<br />
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Fecko: "An integral curve of a vector field V is then the curve γ on M, such that at each point of its image, the equivalence class [γ] given by the curve, coincides with the class V<sub>P</sub>, given by the value of the field V in P. Put another way, from each point it reaches, it moves away exactly in the direction (as well as with the speed) dictated by the vector V<sub>P</sub> . All this may be written as a succinct geometrical equation<br />
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[tex]\dot{\gamma} = V, \enspace\enspace\enspace \text{i.e } \dot{\gamma}(P) = V_P.[/tex]<br />
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"(this is the equation for finding an integral curve γ of a vector field V in a “coordinate-free” form), where the symbol [itex]\dot{\gamma}(P)[/itex] denotes the tangent vector to the curve γ at the point P (i.e. the equivalence class [γ], given by the curve γ at the point P). If the vectors on both sides of this equation are decomposed with respect to a coordinate basis, a system of differential equations for the functions x<sup>i</sup>(t) ≡ x<sup>i</sup>(γ(t)) (for the coordinate presentation of the curve to be found) is obtained."[/tex][/tex]