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Mathematical Methods for Physics and Engineering - Matematica.NET

Mathematical Methods for Physics and Engineering - Matematica.NET

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6.4 CHANGE OF VARIABLES IN MULTIPLE INTEGRALSis constant along the line element KL, the latter has components (∂x/∂u) du <strong>and</strong>(∂y/∂u) du in the directions of the x- <strong>and</strong>y-axes respectively. Similarly, since uis constant along the line element KN, the latter has corresponding components(∂x/∂v) dv <strong>and</strong> (∂y/∂v) dv. Using the result <strong>for</strong> the area of a parallelogram givenin chapter 7, we find that the area of the parallelogram KLMN is given by∣ dA uv =∂x∣ ∂u du∂y ∂x ∂y ∣∣∣dv − dv∂v ∂v ∂u du =∂x ∂y∣ ∂u ∂v − ∂x∂y∂v ∂u∣ du dv.Defining the Jacobian of x, y with respect to u, v as∂(x, y)J =∂(u, v) ≡ ∂x ∂y∂u ∂v − ∂x ∂y∂v ∂u ,we havedA uv =∂(x, y)∣ ∂(u, v) ∣ du dv.The reader acquainted with determinants will notice that the Jacobian can alsobe written as the 2 × 2 determinant∣ ∣∣∣∣∣∣∣ ∂x ∂y∂(x, y)J =∂(u, v) = ∂u ∂u∂x ∂y.∣∂v ∂vSuch determinants can be evaluated using the methods of chapter 8.So, in summary, the relationship between the size of the area element generatedby dx, dy <strong>and</strong> the size of the corresponding area element generated by du, dv isdx dy =∂(x, y)∣ ∂(u, v) ∣ du dv.This equality should be taken as meaning that when trans<strong>for</strong>ming from coordinatesx, y to coordinates u, v, the area element dx dy should be replaced by theexpression on the RHS of the above equality. Of course, the Jacobian can, <strong>and</strong>in general will, vary over the region of integration. We may express the doubleintegral in either coordinate system as∫∫∫∫I = f(x, y) dx dy = g(u, v)∂(x, y)∣RR ∂(u, v) ∣ du dv. (6.12)′When evaluating the integral in the new coordinate system, it is usually advisableto sketch the region of integration R ′ in the uv-plane.201

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