Jacobian matrix and determinant

In vector calculus, the Jacobian matrix (/dʒəˈkoʊbiən/,^[1]^[2]^[3] /dʒɪ-, jɪ-/) of a vector-valued function of several variables is the matrix of all its first-order partial derivatives. When this matrix is square, that is, when the function takes the same number of variables as input as the number of vector components of its output, its determinant is referred to as the Jacobian determinant. Both the matrix and (if applicable) the determinant are often referred to simply as the Jacobian in literature.^[4]

"Jacobian matrix" redirects here. For the operator, see Jacobi matrix (operator).

Definition[edit]

Suppose $f : R n \to R m$ is a function such that each of its first-order partial derivatives exist on $R n$ . This function takes a point $x \in R n$ as input and produces the vector $f (x) \in R m$ as output. Then the Jacobian matrix of $f$ is defined to be an $m \times n$ matrix, denoted by $J$ , whose $(i, j)$ th entry is ${\textstyle \mathbf {J} _{ij}={\frac {\partial f_{i}}{\partial x_{j}}}}$ , or explicitly $\mathbf {J} ={\begin{bmatrix}{\dfrac {\partial \mathbf {f} }{\partial x_{1}}}&\cdots &{\dfrac {\partial \mathbf {f} }{\partial x_{n}}}\end{bmatrix}}={\begin{bmatrix}\nabla ^{\mathrm {T} }f_{1}\\\vdots \\\nabla ^{\mathrm {T} }f_{m}\end{bmatrix}}={\begin{bmatrix}{\dfrac {\partial f_{1}}{\partial x_{1}}}&\cdots &{\dfrac {\partial f_{1}}{\partial x_{n}}}\\\vdots &\ddots &\vdots \\{\dfrac {\partial f_{m}}{\partial x_{1}}}&\cdots &{\dfrac {\partial f_{m}}{\partial x_{n}}}\end{bmatrix}}$ where $\nabla ^{\mathrm {T} }f_{i}$ is the transpose (row vector) of the gradient of the $i$ -th component.

The Jacobian matrix, whose entries are functions of $x$ , is denoted in various ways; common notations include $D f$ , $J f$ , $\nabla \mathbf {f}$ , and ${\frac {\partial (f_{1},..,f_{m})}{\partial (x_{1},..,x_{n})}}$ .^[5]^[6] Some authors define the Jacobian as the transpose of the form given above.

The Jacobian matrix represents the differential of $f$ at every point where $f$ is differentiable. In detail, if $h$ is a displacement vector represented by a column matrix, the matrix product $J (x) \cdot h$ is another displacement vector, that is the best linear approximation of the change of $f$ in a neighborhood of $x$ , if $f (x)$ is differentiable at $x$ .^[a] This means that the function that maps $y$ to $f (x) + J (x) \cdot (y - x)$ is the best linear approximation of $f (y)$ for all points $y$ close to $x$ . The linear map $h \to J (x) \cdot h$ is known as the derivative or the differential of $f$ at $x$ .

When $m = n$ , the Jacobian matrix is square, so its determinant is a well-defined function of $x$ , known as the Jacobian determinant of $f$ . It carries important information about the local behavior of $f$ . In particular, the function $f$ has a differentiable inverse function in a neighborhood of a point $x$ if and only if the Jacobian determinant is nonzero at $x$ (see Jacobian conjecture for a related problem of global invertibility). The Jacobian determinant also appears when changing the variables in multiple integrals (see substitution rule for multiple variables).

When $m = 1$ , that is when $f : R n \to R$ is a scalar-valued function, the Jacobian matrix reduces to the row vector $\nabla ^{\mathrm {T} }f$ ; this row vector of all first-order partial derivatives of $f$ is the transpose of the gradient of $f$ , i.e. $\mathbf {J} _{f}=\nabla ^{T}f$ . Specializing further, when $m = n = 1$ , that is when $f : R \to R$ is a scalar-valued function of a single variable, the Jacobian matrix has a single entry; this entry is the derivative of the function $f$ .

These concepts are named after the mathematician Carl Gustav Jacob Jacobi (1804–1851).

Jacobian matrix[edit]

The Jacobian of a vector-valued function in several variables generalizes the gradient of a scalar-valued function in several variables, which in turn generalizes the derivative of a scalar-valued function of a single variable. In other words, the Jacobian matrix of a scalar-valued function in several variables is (the transpose of) its gradient and the gradient of a scalar-valued function of a single variable is its derivative.

At each point where a function is differentiable, its Jacobian matrix can also be thought of as describing the amount of "stretching", "rotating" or "transforming" that the function imposes locally near that point. For example, if $(x', y') = f (x, y)$ is used to smoothly transform an image, the Jacobian matrix $J f (x, y)$ , describes how the image in the neighborhood of $(x, y)$ is transformed.

If a function is differentiable at a point, its differential is given in coordinates by the Jacobian matrix. However a function does not need to be differentiable for its Jacobian matrix to be defined, since only its first-order partial derivatives are required to exist.

If $f$ is differentiable at a point $p$ in $R n$ , then its differential is represented by $J f (p)$ . In this case, the linear transformation represented by $J f (p)$ is the best linear approximation of $f$ near the point $p$ , in the sense that

$\mathbf {f} (\mathbf {x} )-\mathbf {f} (\mathbf {p} )=\mathbf {J} _{\mathbf {f} }(\mathbf {p} )(\mathbf {x} -\mathbf {p} )+o(\|\mathbf {x} -\mathbf {p} \|)\quad ({\text{as }}\mathbf {x} \to \mathbf {p} ),$

where $o (‖ x - p ‖)$ is a quantity that approaches zero much faster than the distance between $x$ and $p$ does as $x$ approaches $p$ . This approximation specializes to the approximation of a scalar function of a single variable by its Taylor polynomial of degree one, namely

$f(x)-f(p)=f'(p)(x-p)+o(x-p)\quad ({\text{as }}x\to p).$

In this sense, the Jacobian may be regarded as a kind of "first-order derivative" of a vector-valued function of several variables. In particular, this means that the gradient of a scalar-valued function of several variables may too be regarded as its "first-order derivative".

Composable differentiable functions $f : R n \to R m$ and $g : R m \to R k$ satisfy the chain rule, namely $\mathbf {J} _{\mathbf {g} \circ \mathbf {f} }(\mathbf {x} )=\mathbf {J} _{\mathbf {g} }(\mathbf {f} (\mathbf {x} ))\mathbf {J} _{\mathbf {f} }(\mathbf {x} )$ for $x$ in $R n$ .

The Jacobian of the gradient of a scalar function of several variables has a special name: the Hessian matrix, which in a sense is the "second derivative" of the function in question.

Inverse[edit]

According to the inverse function theorem, the matrix inverse of the Jacobian matrix of an invertible function is the Jacobian matrix of the inverse function. That is, if the Jacobian of the function $f : R n \to R n$ is continuous and nonsingular at the point $p$ in $R n$ , then $f$ is invertible when restricted to some neighborhood of $p$ and $\mathbf {J} _{f^{-1}}(x)={\frac {1}{\mathbf {J} _{f}(f^{-1}(x))}}.$

In other words, if the Jacobian determinant is not zero at a point, then the function is locally invertible near this point, that is, there is a neighbourhood of this point in which the function is invertible.

The (unproved) Jacobian conjecture is related to global invertibility in the case of a polynomial function, that is a function defined by n polynomials in n variables. It asserts that, if the Jacobian determinant is a non-zero constant (or, equivalently, that it does not have any complex zero), then the function is invertible and its inverse is a polynomial function.

Examples[edit]

Example 1[edit]

Consider the function $f : R 2 \to R 2,$ with $(x, y) \mapsto (f 1 (x, y), f 2 (x, y)),$ given by $\mathbf {f} \left({\begin{bmatrix}x\\y\end{bmatrix}}\right)={\begin{bmatrix}f_{1}(x,y)\\f_{2}(x,y)\end{bmatrix}}={\begin{bmatrix}x^{2}y\\5x+\sin y\end{bmatrix}}.$

Then we have $f_{1}(x,y)=x^{2}y$ and $f_{2}(x,y)=5x+\sin y$ and the Jacobian matrix of $f$ is $\mathbf {J} _{\mathbf {f} }(x,y)={\begin{bmatrix}{\dfrac {\partial f_{1}}{\partial x}}&{\dfrac {\partial f_{1}}{\partial y}}\\[1em]{\dfrac {\partial f_{2}}{\partial x}}&{\dfrac {\partial f_{2}}{\partial y}}\end{bmatrix}}={\begin{bmatrix}2xy&x^{2}\\5&\cos y\end{bmatrix}}$ and the Jacobian determinant is $\det(\mathbf {J} _{\mathbf {f} }(x,y))=2xy\cos y-5x^{2}.$

Example 2: polar-Cartesian transformation[edit]

The transformation from polar coordinates $(r, φ)$ to Cartesian coordinates (x, y), is given by the function $F : R + \times [0, 2 π) \to R 2$ with components: ${\begin{aligned}x&=r\cos \varphi ;\\y&=r\sin \varphi .\end{aligned}}$ $\mathbf {J} _{\mathbf {F} }(r,\varphi )={\begin{bmatrix}{\frac {\partial x}{\partial r}}&{\frac {\partial x}{\partial \varphi }}\\[0.5ex]{\frac {\partial y}{\partial r}}&{\frac {\partial y}{\partial \varphi }}\end{bmatrix}}={\begin{bmatrix}\cos \varphi &-r\sin \varphi \\\sin \varphi &r\cos \varphi \end{bmatrix}}$

The Jacobian determinant is equal to $r$ . This can be used to transform integrals between the two coordinate systems: $\iint _{\mathbf {F} (A)}f(x,y)\,dx\,dy=\iint _{A}f(r\cos \varphi ,r\sin \varphi )\,r\,dr\,d\varphi .$

Example 3: spherical-Cartesian transformation[edit]

The transformation from spherical coordinates $(ρ, φ, θ)$ ^[7] to Cartesian coordinates (x, y, z), is given by the function $F : R + \times [0, π) \times [0, 2 π) \to R 3$ with components: ${\begin{aligned}x&=\rho \sin \varphi \cos \theta ;\\y&=\rho \sin \varphi \sin \theta ;\\z&=\rho \cos \varphi .\end{aligned}}$

The Jacobian matrix for this coordinate change is $\mathbf {J} _{\mathbf {F} }(\rho ,\varphi ,\theta )={\begin{bmatrix}{\dfrac {\partial x}{\partial \rho }}&{\dfrac {\partial x}{\partial \varphi }}&{\dfrac {\partial x}{\partial \theta }}\\[1em]{\dfrac {\partial y}{\partial \rho }}&{\dfrac {\partial y}{\partial \varphi }}&{\dfrac {\partial y}{\partial \theta }}\\[1em]{\dfrac {\partial z}{\partial \rho }}&{\dfrac {\partial z}{\partial \varphi }}&{\dfrac {\partial z}{\partial \theta }}\end{bmatrix}}={\begin{bmatrix}\sin \varphi \cos \theta &\rho \cos \varphi \cos \theta &-\rho \sin \varphi \sin \theta \\\sin \varphi \sin \theta &\rho \cos \varphi \sin \theta &\rho \sin \varphi \cos \theta \\\cos \varphi &-\rho \sin \varphi &0\end{bmatrix}}.$ The determinant is $ρ 2 sin φ$ . Since $dV = dx dy dz$ is the volume for a rectangular differential volume element (because the volume of a rectangular prism is the product of its sides), we can interpret $dV = ρ 2 sin φ dρ dφ dθ$ as the volume of the spherical differential volume element. Unlike rectangular differential volume element's volume, this differential volume element's volume is not a constant, and varies with coordinates ( $ρ$ and $φ$ ). It can be used to transform integrals between the two coordinate systems: $\iiint _{\mathbf {F} (U)}f(x,y,z)\,dx\,dy\,dz=\iiint _{U}f(\rho \sin \varphi \cos \theta ,\rho \sin \varphi \sin \theta ,\rho \cos \varphi )\,\rho ^{2}\sin \varphi \,d\rho \,d\varphi \,d\theta .$

Example 4[edit]

The Jacobian matrix of the function $F : R 3 \to R 4$ with components ${\begin{aligned}y_{1}&=x_{1}\\y_{2}&=5x_{3}\\y_{3}&=4x_{2}^{2}-2x_{3}\\y_{4}&=x_{3}\sin x_{1}\end{aligned}}$ is $\mathbf {J} _{\mathbf {F} }(x_{1},x_{2},x_{3})={\begin{bmatrix}{\dfrac {\partial y_{1}}{\partial x_{1}}}&{\dfrac {\partial y_{1}}{\partial x_{2}}}&{\dfrac {\partial y_{1}}{\partial x_{3}}}\\[1em]{\dfrac {\partial y_{2}}{\partial x_{1}}}&{\dfrac {\partial y_{2}}{\partial x_{2}}}&{\dfrac {\partial y_{2}}{\partial x_{3}}}\\[1em]{\dfrac {\partial y_{3}}{\partial x_{1}}}&{\dfrac {\partial y_{3}}{\partial x_{2}}}&{\dfrac {\partial y_{3}}{\partial x_{3}}}\\[1em]{\dfrac {\partial y_{4}}{\partial x_{1}}}&{\dfrac {\partial y_{4}}{\partial x_{2}}}&{\dfrac {\partial y_{4}}{\partial x_{3}}}\end{bmatrix}}={\begin{bmatrix}1&0&0\\0&0&5\\0&8x_{2}&-2\\x_{3}\cos x_{1}&0&\sin x_{1}\end{bmatrix}}.$

This example shows that the Jacobian matrix need not be a square matrix.

Example 5[edit]

The Jacobian determinant of the function $F : R 3 \to R 3$ with components ${\begin{aligned}y_{1}&=5x_{2}\\y_{2}&=4x_{1}^{2}-2\sin(x_{2}x_{3})\\y_{3}&=x_{2}x_{3}\end{aligned}}$ is ${\begin{vmatrix}0&5&0\\8x_{1}&-2x_{3}\cos(x_{2}x_{3})&-2x_{2}\cos(x_{2}x_{3})\\0&x_{3}&x_{2}\end{vmatrix}}=-8x_{1}{\begin{vmatrix}5&0\\x_{3}&x_{2}\end{vmatrix}}=-40x_{1}x_{2}.$

From this we see that $F$ reverses orientation near those points where $x 1$ and $x 2$ have the same sign; the function is locally invertible everywhere except near points where $x 1 = 0$ or $x 2 = 0$ . Intuitively, if one starts with a tiny object around the point $(1, 2, 3)$ and apply $F$ to that object, one will get a resulting object with approximately $40 \times 1 \times 2 = 80$ times the volume of the original one, with orientation reversed.

Other uses[edit]

Dynamical systems[edit]

Consider a dynamical system of the form ${\dot {\mathbf {x} }}=F(\mathbf {x} )$ , where ${\dot {\mathbf {x} }}$ is the (component-wise) derivative of $\mathbf {x}$ with respect to the evolution parameter $t$ (time), and $F\colon \mathbb {R} ^{n}\to \mathbb {R} ^{n}$ is differentiable. If $F(\mathbf {x} _{0})=0$ , then $\mathbf {x} _{0}$ is a stationary point (also called a steady state). By the Hartman–Grobman theorem, the behavior of the system near a stationary point is related to the eigenvalues of $\mathbf {J} _{F}\left(\mathbf {x} _{0}\right)$ , the Jacobian of $F$ at the stationary point.^[8] Specifically, if the eigenvalues all have real parts that are negative, then the system is stable near the stationary point. If any eigenvalue has a real part that is positive, then the point is unstable. If the largest real part of the eigenvalues is zero, the Jacobian matrix does not allow for an evaluation of the stability.^[9]

Newton's method[edit]

A square system of coupled nonlinear equations can be solved iteratively by Newton's method. This method uses the Jacobian matrix of the system of equations.

Regression and least squares fitting[edit]

The Jacobian serves as a linearized design matrix in statistical regression and curve fitting; see non-linear least squares. The Jacobian is also used in random matrices, moments, local sensitivity and statistical diagnostics.^[10]^[11]

Center manifold

Hessian matrix

Pushforward (differential)

(1996). "Comparative Statics and the Correspondence Principle". Economic Dynamics (Third ed.). Berlin: Springer. pp. 305–330. ISBN 3-540-60988-1.

Gandolfo, Giancarlo

; Morrey, Charles B. Jr. (1985). "Transformations and Jacobians". Intermediate Calculus (Second ed.). New York: Springer. pp. 412–420. ISBN 0-387-96058-9.