mathematical-analysis mathematics real-mathematical-analysis vector-mathematical-analysis Taylor Expansion (Real Scalar Fields) Definition: Taylor Polynomial
TODO
Theorem: Taylor Polynomial via Partial Derivatives
Let \(f: \mathcal{D} \subseteq \mathbb{R}^n \to \mathbb{R}\) be a real scalar field .
If \(f\) is \(m\) -times totally differentiable at \(\boldsymbol{p} \in \operatorname{int} \mathcal{D}\) , then its Taylor polynomial there is given by \(f\) 's partial derivatives as follows:
\[T(\boldsymbol{p}; \boldsymbol{x}) = f(\boldsymbol{p}) + \sum_{k = 1}^m \frac{1}{k!}\left(\sum_{i_1 = 1}^n\cdots \sum_{i_k = 1}^n \partial_{i_1}\cdots \partial_{i_k}f(\boldsymbol{p}) \prod_{j = 1}^k (x_{i_j} - p_{i_j})\right)\]
Tip
This formula can be rewritten using \(f\) 's gradient and Hessian matrix as follows:
\[T(\boldsymbol{p}; \boldsymbol{x}) = f(\boldsymbol{p}) + \nabla f(\boldsymbol{p})^{\mathsf{T}}(\boldsymbol{x}-\boldsymbol{p}) + \frac{1}{2} (\boldsymbol{x}-\boldsymbol{p})^{\mathsf{T}} \boldsymbol{H}_f(\boldsymbol{p})(\boldsymbol{x}-\boldsymbol{p}) + \sum_{k = 3}^m \frac{1}{k!}\left(\sum_{i_1 = 1}^n\cdots \sum_{i_k = 1}^n \partial_{i_1}\cdots \partial_{i_k}f(\boldsymbol{p}) \prod_{j = 1}^k (x_{i_j} - p_{i_j})\right)\]
Proof TODO
Theorem: Lagrange Form of the Remainder
Let \(f: \mathcal{D} \subseteq \mathbb{R}^n \to \mathbb{R}\) be a real scalar field and let \(\boldsymbol{p},\boldsymbol{x} \in \mathcal{D}\) .
If \(f\) is \((m+1)\) -times totally differentiable on an open set which contains \(L = \{\boldsymbol{p} + t(\boldsymbol{x} -\boldsymbol{p}): t \in [0,1]\}\) , then there exists some \(\boldsymbol{\xi} \in \operatorname{int} L\) such that the remainder \(R_{m+1}(\boldsymbol{p}; \boldsymbol{x})\) of \(f\) 's \(m\) -th Taylor polynomial \(T_m(\boldsymbol{p};\boldsymbol{x})\) is given by \(f\) 's partial derivatives as follows:
\[R_{m+1}(\boldsymbol{p}; \boldsymbol{x}) = \frac{1}{(m+1)!} \left(\sum_{i_1 = 1}^n\cdots \sum_{i_{m+1} = 1}^n \partial_{i_1}\cdots \partial_{i_{m+1}}f(\boldsymbol{\xi}) \prod_{j = 1}^{m+1} (x_{i_j} - p_{i_j})\right),\]
Proof TODO
Theorem: Integral Form of the Remainder
Let \(f: \mathcal{D} \subseteq \mathbb{R}^n \to \mathbb{R}\) be a real scalar field and let \(\boldsymbol{p}, \boldsymbol{x} \in \mathcal{D}\) .
If \(f\) is \((m+1)\) -times continuously partially differentiable on an open set which contains \(L = \{\boldsymbol{p} + t(\boldsymbol{x} -\boldsymbol{p}): t \in [0,1]\}\) , then the remainder \(R_{m+1}(\boldsymbol{p}; \boldsymbol{x})\) of \(f\) 's \(m\) -th Taylor polynomial \(T_m(\boldsymbol{p};\boldsymbol{x})\) is given by the following integral :
\[R_{m+1}(\boldsymbol{p}; \boldsymbol{x}) = \frac{1}{m!}\int_0^1 (1-t)^m \left(\sum_{i_1 = 1}^n\cdots \sum_{i_{m+1} = 1}^n \partial_{x^{i_1}}\cdots \partial_{x^{i_{m+1}}}f(\boldsymbol{p} + t(\boldsymbol{x} - \boldsymbol{p})) \prod_{j = 1}^{m+1} (x^{i_j} - p^{i_j})\right)\,\mathrm{d}t\]
Proof TODO
Theorem: Remainder and Bachmann-Landau Notation
Let \(f: \mathcal{D} \subseteq \mathbb{R}^n \to \mathbb{R}\) be a real scalar field and let \(\boldsymbol{p} \in \mathcal{D}\) .
If \(f\) is \(m\) -times totally differentiable at \(\boldsymbol{p}\) , then the remainder \(R_{m+1}(\boldsymbol{p}; \boldsymbol{x}) = f(\boldsymbol{x}) - T_m(\boldsymbol{p};\boldsymbol{x})\) of \(f\) 's \(m\) -th Taylor polynomial \(T_m(\boldsymbol{p};\boldsymbol{x})\) is little o of \(||\boldsymbol{x} - \boldsymbol{p}||^m\) for \(\boldsymbol{x} \to \boldsymbol{p}\) :
\[R_{m+1}(\boldsymbol{p}; \boldsymbol{x}) = o(||\boldsymbol{x} - \boldsymbol{p}||^m) \qquad \text{for} \qquad \boldsymbol{x} \to \boldsymbol{p}\]
If \(f\) is \((m+1)\) -times continuously partially differentiable on an open neighborhood of \(\boldsymbol{p}\) , then the remainder \(R_{m+1}(\boldsymbol{p}; \boldsymbol{x}) = f(\boldsymbol{x}) - T_m(\boldsymbol{p};\boldsymbol{x})\) of \(f\) 's \(m\) -th Taylor polynomial \(T_m(\boldsymbol{p};\boldsymbol{x})\) is Big O of \(||\boldsymbol{x} - \boldsymbol{p}||^{m+1}\) for \(\boldsymbol{x} \to \boldsymbol{p}\) :
\[R_{m+1}(\boldsymbol{p}; \boldsymbol{x}) = O(||\boldsymbol{x} - \boldsymbol{p}||^{m+1}) \qquad \text{for} \qquad \boldsymbol{x} \to \boldsymbol{p}\]
Example: \(f(x, y) = x^3 \mathrm{e}^{y}\) Consider the real scalar field \(f: \mathbb{R}^2 \to \mathbb{R}\) defined as follows:
\[f\left(x, y\right) = x^3 \mathrm{e}^{y}\]
For its partial derivatives , we have:
\[\partial_{x}f(x, y) = 3x^2 \mathrm{e}^{y} \qquad \partial_{y}f(x, y) = x^3 \mathrm{e}^{y}\]
\[\partial_{x}\partial_{x}f(x, y) = 6x \mathrm{e}^{y} \qquad \partial_{x}\partial_{y}f(x, y) = 3x^2 \mathrm{e}^{y} = \partial_{y}\partial_{x}f(x, y) \qquad \partial_{y}\partial_{y}f(x, y) = x^3 \mathrm{e}^{y}\]
Therefore:
\[f\left(\begin{bmatrix}1 \\ 0\end{bmatrix}\right) = 1 \qquad \nabla f\left(\begin{bmatrix}1 \\ 0\end{bmatrix}\right) = \begin{bmatrix}3 \\ 1\end{bmatrix} \qquad H_f\left(\begin{bmatrix}1 \\ 0\end{bmatrix}\right) = \begin{bmatrix}6 & 3 \\ 3 & 1\end{bmatrix}\]
We thus have:
\[\begin{aligned}f\left(x, y\right) & = T_2\left(\begin{bmatrix}1 \\ 0\end{bmatrix}; \begin{bmatrix}x \\ y\end{bmatrix}\right) + R_3\left(\begin{bmatrix}1 \\ 0\end{bmatrix}; \begin{bmatrix}x \\ y\end{bmatrix}\right) \\ & = f\left(\begin{bmatrix}1 \\ 0\end{bmatrix}\right) + \nabla f\left(\begin{bmatrix}1 \\ 0\end{bmatrix}\right)^{\mathsf{T}}\left(\begin{bmatrix}x \\ y\end{bmatrix}-\begin{bmatrix}1 \\ 0\end{bmatrix}\right) + \frac{1}{2}\left(\begin{bmatrix}x \\ y\end{bmatrix}-\begin{bmatrix}1 \\ 0\end{bmatrix}\right)^{\mathsf{T}} H_f\left(\begin{bmatrix}1 \\ 0\end{bmatrix}\right) \left(\begin{bmatrix}x \\ y\end{bmatrix}-\begin{bmatrix}1 \\ 0\end{bmatrix}\right) + R_3\left(\begin{bmatrix}1 \\ 0\end{bmatrix}; \begin{bmatrix}x \\ y\end{bmatrix}\right) \\ & = f\left(\begin{bmatrix}1 \\ 0\end{bmatrix}\right) + \begin{bmatrix}3 & 1\end{bmatrix}\left(\begin{bmatrix}x \\ y\end{bmatrix}-\begin{bmatrix}1 \\ 0\end{bmatrix}\right) + \frac{1}{2}\left(\begin{bmatrix}x \\ y\end{bmatrix}-\begin{bmatrix}1 \\ 0\end{bmatrix}\right)^{\mathsf{T}}\begin{bmatrix}6 & 3 \\ 3 & 1\end{bmatrix}\left(\begin{bmatrix}x \\ y\end{bmatrix}-\begin{bmatrix}1 \\ 0\end{bmatrix}\right) + O\left(\left\vert\left\vert \begin{bmatrix}x \\ y\end{bmatrix} - \begin{bmatrix}1 \\ 0\end{bmatrix}\right\vert\right\vert^3\right) \qquad \text{for} \qquad \begin{bmatrix}x \\ y\end{bmatrix} \to \begin{bmatrix}1 \\ 0\end{bmatrix} \\ & = f\left(\begin{bmatrix} 1 \\ 0 \end{bmatrix}\right) + 3(x - 1) + y + 3(x - 1)^2 + 3(x - 1)y + \frac{1}{2}y^2 + O\left(\left((x-1)^2 + y^2\right)^{3/2}\right)\end{aligned}\]
Proof TODO
April 3, 2026 April 3, 2026