Difference between revisions of "Leibniz rule"
(Redirected page to Derivation in a ring) |
|||
Line 1: | Line 1: | ||
− | + | {{MSC|26A06|26B05}} | |
+ | |||
+ | {{MSC|58A05}} | ||
+ | |||
+ | {{MSC|12H05}} | ||
+ | {{TEX|done}} | ||
+ | |||
+ | ''product rule'' | ||
+ | |||
+ | In calculus, the term refers to the elementary rule for the [[Derivative|derivative]] of the product of two functions. In its simplest form it states the following | ||
+ | |||
+ | '''Theorem 1''' | ||
+ | Let $I$ be an open interval and $x_0\in I$. Let $f,g : I \to \mathbb R$ be two functions which are [[Differentiable function|differentiable]] at $x_0$. Then $fg$ is also differentiable at $x_0$ and | ||
+ | \begin{equation}\label{e:rule} | ||
+ | (fg)' (x_0) = f(x_0) g'(x_0) + f' (x_0) g (x_0)\, . | ||
+ | \end{equation} | ||
+ | |||
+ | ====Variants==== | ||
+ | The same rule applies also to several other situations. The following is a list of rather important cases. | ||
+ | * $x_0\in U$ open subset of $\mathbb R^n$ and the maps $f,g: U \to \mathbb R$ have both the [[Partial derivative|partial derivative]] $\frac{\partial}{\partial x_i}$ at $x_0$. The corresponding formula is then | ||
+ | \[ | ||
+ | \frac{\partial}{\partial x_i} (fg) (x_0) = g(x_0) \frac{\partial f}{\partial x_i} (x_0) + f(x_0) \frac{\partial g}{\partial x_i} (x_0)\, . | ||
+ | \] | ||
+ | * $x_0\in U$ open subset of $\mathbb R^n$, or more generally $x_0\in M$ for some [[Differentiable manifold|differentiable manifold]], and the maps $f,g U \to \mathbb R$ are differentiable along a [[Vector field on a manifold|vector field]]. The rule becomes then | ||
+ | \[ | ||
+ | [X (fg)]\, (x_0) = g (x_0)\, [X (f)]\, (x_0) + f(x_0)\, [X (g)]\, (x_0)\, . | ||
+ | \] | ||
+ | * $x_0\in U$ open subset of $\mathbb R^n$, or more generally $x_0\in M$ for some [[Differentiable manifold|differentiable manifold]], and the maps $f,g: U \to \mathbb R$ are differentiable. The formula is then | ||
+ | \[ | ||
+ | \left. d (fg) \right|_{x_0} = f(x_0)\, \left. dg\right|_{x_0} + g(x_0)\, \left. df\right|_{x_0}\, . | ||
+ | \] | ||
+ | * $z_0\in U$ open subset of $\mathbb C$ and $f,g: U \to \mathbb C$ are differentiable in the sense of complex analysis (cf. [[Analytic function]]). Then the formula reads as \eqref{e:rule}. | ||
+ | |||
+ | ====Algebraic generalizations==== | ||
+ | The Leibniz rule is, together with the linearity, the key algebraic identity which unravels most of the structural properties of the differentiation. For this reason, in several situations people call ''derivations'' those operations over an appropriate set of functions which are linear and satisfy the Leibniz rule. Two important instances are: | ||
+ | |||
+ | * [[Derivation in a ring]]. The primary example is the following: given a [[Differentiable manifold|differentiable manifold]] $M$, consider the [[Ring|ring]] $C^1 (M)$ of $C^1$ real-valued functions over $M$. A derivation at $x_0$ is a map $D: C^1 (M) \to \mathbb R$ which is linear, i.e. | ||
+ | \[ | ||
+ | D (\lambda f + \mu g) = \lambda Df + \mu Dg \qquad \forall \lambda, \mu \in \mathbb R, \forall f,g\in C^1 (M)\, , | ||
+ | \] | ||
+ | and satisfies the Leibniz rule, i.e. | ||
+ | \[ | ||
+ | D (fg) = f(x_0) Dg + g (x_0) Df\, . | ||
+ | \] | ||
+ | Global derivatives are maps from $C^1 (M)$ to $C^0 (M)$ satisfying the (analog of) the same rules. Derivations give one way (among many equivalent others) to define the [[Tangent space|tangent space]] to differentiable manifolds and [[Vector field on a manifold|vector fields]] on them (together with the [[Lie bracket]]). | ||
+ | *[[Differential field]]. A field $\mathbb F$ with a map $':\mathbb F \to \mathbb F$ (called derivation) satisfying the rules | ||
+ | \[ | ||
+ | (f+g)' = f' + g' \qquad \mbox{and} \qquad (fg)' = fg' + gf'\, . | ||
+ | \] | ||
+ | Differential fields are the object of study of [[Differential algebra]]. Historically the birth of differential algebra can be dated back to the following famous theorem of Liouville ({{Cite|Li}}): the [[Primitive function|primitive]] of $e^{x^2}$ cannot be expressed in terms of [[Elementary functions|elementary functions]] (see {{Cite|Ro}} for a modern proof). | ||
+ | |||
+ | ====References==== | ||
+ | {| | ||
+ | |- | ||
+ | |valign="top"|{{Ref|Ca}}|| H. Cartan, "Elementary Theory of Analytic Functions of One or Several Complex Variable", Dover (1995). | ||
+ | |- | ||
+ | |valign="top"|{{Ref|Li}}|| J. Liouville, "Mémoire sur les Trascendantes Elliptiques et sur l’impossibilité d’exprimer les racines de certaines équations en fonction finie explicite des coefficients", ''J. Math. Pures Appl.'' '''2''' (1837) pp. 124–193. | ||
+ | |- | ||
+ | |valign="top"|{{Ref|Ma}}|| A. R. Magid, "Lectures on differential Galois theory", ''University Lecture Series, 7.'' American Mathematical Society, Providence, RI, (1994) | ||
+ | |- | ||
+ | |valign="top"|{{Ref|Ro}}|| M. Rosenlicht, "Integration in finite terms", ''Amer. Math. Monthly'' '''79''' (1972) pp. 963–972. | ||
+ | |- | ||
+ | |valign="top"|{{Ref|Ru}}|| W. Rudin, "Principles of mathematical analysis" , McGraw-Hill (1976) {{MR|0385023}} {{ZBL|0346.26002}} | ||
+ | |- | ||
+ | |valign="top"|{{Ref|Sp}}|| M. Spivak, "Calculus on manifolds" , Benjamin (1965) | ||
+ | |- | ||
+ | |} |
Revision as of 10:17, 11 December 2013
2020 Mathematics Subject Classification: Primary: 26A06 Secondary: 26B05 [MSN][ZBL]
2020 Mathematics Subject Classification: Primary: 58A05 [MSN][ZBL]
2020 Mathematics Subject Classification: Primary: 12H05 [MSN][ZBL]
product rule
In calculus, the term refers to the elementary rule for the derivative of the product of two functions. In its simplest form it states the following
Theorem 1 Let $I$ be an open interval and $x_0\in I$. Let $f,g : I \to \mathbb R$ be two functions which are differentiable at $x_0$. Then $fg$ is also differentiable at $x_0$ and \begin{equation}\label{e:rule} (fg)' (x_0) = f(x_0) g'(x_0) + f' (x_0) g (x_0)\, . \end{equation}
Variants
The same rule applies also to several other situations. The following is a list of rather important cases.
- $x_0\in U$ open subset of $\mathbb R^n$ and the maps $f,g: U \to \mathbb R$ have both the partial derivative $\frac{\partial}{\partial x_i}$ at $x_0$. The corresponding formula is then
\[ \frac{\partial}{\partial x_i} (fg) (x_0) = g(x_0) \frac{\partial f}{\partial x_i} (x_0) + f(x_0) \frac{\partial g}{\partial x_i} (x_0)\, . \]
- $x_0\in U$ open subset of $\mathbb R^n$, or more generally $x_0\in M$ for some differentiable manifold, and the maps $f,g U \to \mathbb R$ are differentiable along a vector field. The rule becomes then
\[ [X (fg)]\, (x_0) = g (x_0)\, [X (f)]\, (x_0) + f(x_0)\, [X (g)]\, (x_0)\, . \]
- $x_0\in U$ open subset of $\mathbb R^n$, or more generally $x_0\in M$ for some differentiable manifold, and the maps $f,g: U \to \mathbb R$ are differentiable. The formula is then
\[ \left. d (fg) \right|_{x_0} = f(x_0)\, \left. dg\right|_{x_0} + g(x_0)\, \left. df\right|_{x_0}\, . \]
- $z_0\in U$ open subset of $\mathbb C$ and $f,g: U \to \mathbb C$ are differentiable in the sense of complex analysis (cf. Analytic function). Then the formula reads as \eqref{e:rule}.
Algebraic generalizations
The Leibniz rule is, together with the linearity, the key algebraic identity which unravels most of the structural properties of the differentiation. For this reason, in several situations people call derivations those operations over an appropriate set of functions which are linear and satisfy the Leibniz rule. Two important instances are:
- Derivation in a ring. The primary example is the following: given a differentiable manifold $M$, consider the ring $C^1 (M)$ of $C^1$ real-valued functions over $M$. A derivation at $x_0$ is a map $D: C^1 (M) \to \mathbb R$ which is linear, i.e.
\[ D (\lambda f + \mu g) = \lambda Df + \mu Dg \qquad \forall \lambda, \mu \in \mathbb R, \forall f,g\in C^1 (M)\, , \] and satisfies the Leibniz rule, i.e. \[ D (fg) = f(x_0) Dg + g (x_0) Df\, . \] Global derivatives are maps from $C^1 (M)$ to $C^0 (M)$ satisfying the (analog of) the same rules. Derivations give one way (among many equivalent others) to define the tangent space to differentiable manifolds and vector fields on them (together with the Lie bracket).
- Differential field. A field $\mathbb F$ with a map $':\mathbb F \to \mathbb F$ (called derivation) satisfying the rules
\[ (f+g)' = f' + g' \qquad \mbox{and} \qquad (fg)' = fg' + gf'\, . \] Differential fields are the object of study of Differential algebra. Historically the birth of differential algebra can be dated back to the following famous theorem of Liouville ([Li]): the primitive of $e^{x^2}$ cannot be expressed in terms of elementary functions (see [Ro] for a modern proof).
References
[Ca] | H. Cartan, "Elementary Theory of Analytic Functions of One or Several Complex Variable", Dover (1995). |
[Li] | J. Liouville, "Mémoire sur les Trascendantes Elliptiques et sur l’impossibilité d’exprimer les racines de certaines équations en fonction finie explicite des coefficients", J. Math. Pures Appl. 2 (1837) pp. 124–193. |
[Ma] | A. R. Magid, "Lectures on differential Galois theory", University Lecture Series, 7. American Mathematical Society, Providence, RI, (1994) |
[Ro] | M. Rosenlicht, "Integration in finite terms", Amer. Math. Monthly 79 (1972) pp. 963–972. |
[Ru] | W. Rudin, "Principles of mathematical analysis" , McGraw-Hill (1976) MR0385023 Zbl 0346.26002 |
[Sp] | M. Spivak, "Calculus on manifolds" , Benjamin (1965) |
Leibniz rule. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Leibniz_rule&oldid=26602