Today in Physics 217: Vector Derivatives
Today in Physics 217: vector derivatives First derivatives: • Gradient (—) • Divergence (—◊) •Curl (—¥) Second derivatives: the Laplacian (—2) and its relatives Vector-derivative identities: relatives of the chain rule, product rule, etc. Image by Eric Carlen, School of Mathematics, Georgia Institute of 22 vxyxy, =−++ x yˆˆ x y Technology ()()() 6 September 2002 Physics 217, Fall 2002 1 Differential vector calculus df/dx provides us with information on how quickly a function of one variable, f(x), changes. For instance, when the argument changes by an infinitesimal amount, from x to x+dx, f changes by df, given by df df= dx dx In three dimensions, the function f will in general be a function of x, y, and z: f(x, y, z). The change in f is equal to ∂∂∂fff df=++ dx dy dz ∂∂∂xyz ∂∂∂fff =++⋅++ˆˆˆˆˆˆ xyzxyz ()()dx() dy() dz ∂∂∂xyz ≡⋅∇fdl 6 September 2002 Physics 217, Fall 2002 2 Differential vector calculus (continued) The vector derivative operator — (“del”) ∂∂∂ ∇ =++xyzˆˆˆ ∂∂∂xyz produces a vector when it operates on scalar function f(x,y,z). — is a vector, as we can see from its behavior under coordinate rotations: I ′ ()∇∇ff=⋅R but its magnitude is not a number: it is an operator. 6 September 2002 Physics 217, Fall 2002 3 Differential vector calculus (continued) There are three kinds of vector derivatives, corresponding to the three kinds of multiplication possible with vectors: Gradient, the analogue of multiplication by a scalar. ∇f Divergence, like the scalar (dot) product. ∇⋅v Curl, which corresponds to the vector (cross) product. ∇×v 6 September 2002 Physics 217, Fall 2002 4 Gradient The result of applying the vector derivative operator on a scalar function f is called the gradient of f: ∂∂∂fff ∇f =++xyzˆˆˆ ∂∂∂xyz The direction of the gradient points in the direction of maximum increase of f (i.e.
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