Power series of a function of 2 variables

[Castilla]

I have learned that if a function of one real variable can be defined as a power series, then this one is its Taylor series.

Does the same occur with functions of 2 real variables? I mean, if a function f(x, y) can be defined as a power series, does this series is the Taylor series of f(x, y)?

Thanks for help.

 

[CompuChip]

I thought an expansion like this was possible...
<br /> f(x, y) = f(x_0, y_0) <br /> + \left. \frac{\partial f(x, y_0)}{\partial x} \right|_{x = x_0} (x - x_0)<br /> + \left. \frac{\partial f(x_0, y)}{\partial x} \right|_{y = y_0} (y - y_0)<br /> + \frac12 \left. \frac{\partial^2 f(x, y_0)}{\partial x^2} \right|_{x = x_0} (x - x_0)^2 <br /><br /> + \frac12 \left. \frac{\partial^2 f(x_0, y)}{\partial y^2} \right|_{y = y_0} (y - y_0)^2<br /> + \frac12 \left. \frac{\partial^2 f(x, y)}{\partial x \partial y}(x-x_0)(y-y_0) \cdots<br /> + \mathcal{O}(x, y)^3<br />

 

[HallsofIvy]

That should be
<br /> f(x, y) = f(x_0, y_0) <br /> + \left. \frac{\partial f(x, y_0)}{\partial x} \right|_{x = x_0} (x - x_0)<br /> + \left. \frac{\partial f(x_0, y)}{\partial x} \right|_{y = y_0} (y - y_0)<br /> + \frac12 \left. \frac{\partial^2 f(x, y_0)}{\partial x^2} \right|_{x = x_0} (x - x_0)^2 <br /><br /> + \frac12 \left. \frac{\partial^2 f(x_0, y)}{\partial y^2} \right|_{y = y_0} (y - y_0)^2<br /> + \frac12 \left. \frac{\partial^2 f(x, y)}{\partial x \partial y}(x-x_0)(y-y_0)\cdots<br /> + \mathcal{O}(x, y)^3<br />
where I have added (x-x_0)(y-y_0) after the mixed second derivative.

 

[CompuChip]

I believe that's what I meant by the \cdots, sorry for being unclear.

 

[arildno]

This is incorrect, Halls!
You have a 1/2 in front of the mixed second partial; it should be a 1 instead.

For OP:
Here's how we can DEDUCE the look of the Taylor polynomial for a 2-variable function.
Now, given a function f(x,y); we may as a first step regard this as a single variable function G(x;y)=f(x,y); where "y" in G is just some fixed parameter.
G can be expanded in a 1-variable Taylor series in x about the point (x0,y), so switching to f-notation, we have:
f(x,y)=\sum_{n=0}^{\infty}\frac{1}{n!}\frac{\partial^{n}f}{\partial{x}^{n}}(x_{0},y)(x-x_{0})^{n}
where the 0'th derivative of a function means the function itself.

Now, each of these derivatives is a function of y, with a fixed parameter x0. Thus, they can be expanded as Taylor series, and we get:
f(x,y)=\sum_{n=0}^{\infty}\frac{1}{n!}\sum_{m=0}^{\infty}\frac{1}{m!}\frac{\partial^{(n+m)}f}{\partial{x}^{n}\partial{y}^{m}}(x_{0},y_{0})(x-x_{0})^{n}(y-y_{0})^{m}
Regrouping our double series in term of the total derivative index s=n+m, we readily get:
f(x,y)=\sum_{s=0}^{\infty}\frac{1}{s!}\sum_{n=0}^{s}\binom{s}{n}\frac{\partial^{s}f}{\partial{x}^{n}\partial{y}^{(s-n)}}(x_{0},y_{0})(x-x_{0})^{n}(y-y_{0})^{(s-n)}
where I have utilized \frac{1}{s!}\binom{s}{n}=\frac{1}{n!}\frac{1}{(s-n)!}


This form is readily extendable to functions with more than two variables as well.

 

[jostpuur]

One easy way to remember the Taylor series in higher dimensions is to write it like

<br /> f(x+u) = f(x)\; +\; u\cdot\nabla f(x)\; +\; \frac{1}{2!}(u\cdot\nabla)^2 f(x)\; +\; \frac{1}{3!}(u\cdot\nabla)^3 f(x)\; + \cdots<br />

You can get those coefficients for the partial derivatives by computing (u\cdot\nabla)^n open. For example

<br /> (u_1\partial_1 + u_2\partial_2)^2 = u_1^2\partial_1^2 + 2u_1u_2\partial_1\partial_2 + u_2^2\partial_2^2<br />