Difference between revisions of "Differential parameter"
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''differentiator'' | ''differentiator'' | ||
− | The joint [[Differential invariant|differential invariant]] of one or more functions and the metric tensor | + | The joint [[Differential invariant|differential invariant]] of one or more functions and the metric tensor $g_{ij}$ of a Riemannian geometry. |
− | The first-order differential parameter (or simply differential parameter) of a function | + | The first-order differential parameter (or simply differential parameter) of a function $V$ is the square of its gradient: |
− | + | $$\Delta_1V=g^{ij}V_iV_j.$$ | |
− | The first-order mixed differential parameter of two functions | + | The first-order mixed differential parameter of two functions $V$ and $W$ is the scalar product of their gradients |
− | + | $$\Delta_1(V,W)=g^{ij}V_iW_j.$$ | |
In three-dimensional Euclidean space and with respect to a Cartesian rectangular coordinate system these differential parameters are given by the formulas | In three-dimensional Euclidean space and with respect to a Cartesian rectangular coordinate system these differential parameters are given by the formulas | ||
− | + | $$\Delta_1(V)=\left(\frac{\partial V}{\partial x}\right)^2+\left(\frac{\partial V}{\partial y}\right)^2+\left(\frac{\partial V}{\partial z}\right)^2,$$ | |
− | + | $$\Delta_1(V,W)=\frac{\partial V}{\partial x}\frac{\partial W}{\partial x}+\frac{\partial V}{\partial y}\frac{\partial W}{\partial y}+\frac{\partial V}{\partial z}\frac{\partial W}{\partial z}.$$ | |
The second-order differential parameter (or second differential parameter) of a function is the divergence of its gradient: | The second-order differential parameter (or second differential parameter) of a function is the divergence of its gradient: | ||
− | + | $$\Delta_2(V)=g^{ij}\nabla_iV_j=\frac{1}{\sqrt g}\frac{\partial}{\partial x^i}(\sqrt{gg}^{ij}V_j),$$ | |
− | where | + | where $g$ is the determinant of the matrix $\|g_{ij}\|$. In three-dimensional Euclidean space and with respect to a Cartesian rectangular coordinate system, the second differential parameter is given by the formula |
− | + | $$\Delta_2(V)=\frac{\partial^2V}{\partial x^2}+\frac{\partial^2V}{\partial y^2}+\frac{\partial^2V}{\partial z^2}.$$ | |
Differential parameters were first introduced by G. Lamé [[#References|[1]]] in Euclidean geometry. E. Beltrami [[#References|[2]]] must be credited with generalizing this concept. The differential parameters are therefore sometimes called Lamé or Beltrami differential parameters. | Differential parameters were first introduced by G. Lamé [[#References|[1]]] in Euclidean geometry. E. Beltrami [[#References|[2]]] must be credited with generalizing this concept. The differential parameters are therefore sometimes called Lamé or Beltrami differential parameters. |
Latest revision as of 08:18, 23 August 2014
differentiator
The joint differential invariant of one or more functions and the metric tensor $g_{ij}$ of a Riemannian geometry.
The first-order differential parameter (or simply differential parameter) of a function $V$ is the square of its gradient:
$$\Delta_1V=g^{ij}V_iV_j.$$
The first-order mixed differential parameter of two functions $V$ and $W$ is the scalar product of their gradients
$$\Delta_1(V,W)=g^{ij}V_iW_j.$$
In three-dimensional Euclidean space and with respect to a Cartesian rectangular coordinate system these differential parameters are given by the formulas
$$\Delta_1(V)=\left(\frac{\partial V}{\partial x}\right)^2+\left(\frac{\partial V}{\partial y}\right)^2+\left(\frac{\partial V}{\partial z}\right)^2,$$
$$\Delta_1(V,W)=\frac{\partial V}{\partial x}\frac{\partial W}{\partial x}+\frac{\partial V}{\partial y}\frac{\partial W}{\partial y}+\frac{\partial V}{\partial z}\frac{\partial W}{\partial z}.$$
The second-order differential parameter (or second differential parameter) of a function is the divergence of its gradient:
$$\Delta_2(V)=g^{ij}\nabla_iV_j=\frac{1}{\sqrt g}\frac{\partial}{\partial x^i}(\sqrt{gg}^{ij}V_j),$$
where $g$ is the determinant of the matrix $\|g_{ij}\|$. In three-dimensional Euclidean space and with respect to a Cartesian rectangular coordinate system, the second differential parameter is given by the formula
$$\Delta_2(V)=\frac{\partial^2V}{\partial x^2}+\frac{\partial^2V}{\partial y^2}+\frac{\partial^2V}{\partial z^2}.$$
Differential parameters were first introduced by G. Lamé [1] in Euclidean geometry. E. Beltrami [2] must be credited with generalizing this concept. The differential parameters are therefore sometimes called Lamé or Beltrami differential parameters.
References
[1] | G. Lamé, "Leçons sur les coordonnées curvilignes et leurs diverses applications" , Paris (1958) |
[2] | E. Betrami, "Ricerche di analisi applicate alla geometria" G. Mat. Battaglini , 2–3 (1864–1865) |
[3] | V.F. Kagan, "Foundations of the theory of surfaces in a tensor setting" , 1–2 , Moscow-Leningrad (1947–1948) (In Russian) |
[4] | V.I. Shulikovskii, "Classical differential geometry in a tensor setting" , Moscow (1963) (In Russian) |
Comments
References
[a1] | J.J. Stoker, "Differential geometry" , Wiley (Interscience) (1969) |
Differential parameter. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Differential_parameter&oldid=11879