1 / 6

Calculus III

Calculus III. Chapter 13. Partial Derivatives of f(x,y). Tangent Plane and the Differential. The tangent plane to the surface z = f(x,y): The tangent plane approximation: The differential:

tarika
Download Presentation

Calculus III

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. Calculus III Chapter 13

  2. Partial Derivatives of f(x,y) • . • .

  3. Tangent Plane and the Differential • The tangent plane to the surface z = f(x,y): • The tangent plane approximation: • The differential: • For a function z = f(x,y), the differential, df, at a point (a,b) is the linear function of dx and dy given by the formula:

  4. The Gradient of z = f(x,y) • If f is a differentiable function at the point (a,b) and f (a,b)  0, then: • The direction of f (a,b) is • Perpendicular to the contour of f through (a,b) • In the direction of increasing f • The magnitude of the gradient vector, || f ||, is • The maximum rate of change of at that point • Large when the contours are close together and small when they are far apart.

  5. The Gradient of w = f(x,y,z) Properties: • The direction of the gradient vector is the direction in which f is increasing at the greatest rate, if it exists. • The magnitude, ||grad f||, is the rate of change of f in that direction. • If the directional derivative of f at (a,b,c) is zero in all directions then the grad f is defined to be 0.

  6. Differentiability • For a function f at a point (a,b), let E(x,y) be the error in the local linear approximation, that is the absolute value of the difference between the left and right hand sides, and let d(x,y) be the distance between (x,y) and (a,b). Then f is said to be locally linear, or differentiable at (a,b) if we can make the ratio E(x,y)/d(x,y) as small as we like by restricting (x,y) to a small enough non-zero distance from (a,b).

More Related