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Chapter 16 – Vector Calculus 16.1 Vector Fields 1 Objectives:  Understand the different types of vector fields Dr. Erickson.

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Presentation on theme: "Chapter 16 – Vector Calculus 16.1 Vector Fields 1 Objectives:  Understand the different types of vector fields Dr. Erickson."— Presentation transcript:

1 Chapter 16 – Vector Calculus 16.1 Vector Fields 1 Objectives:  Understand the different types of vector fields Dr. Erickson

2 Vector Calculus In this chapter, we study the calculus of vector fields. ◦ These are functions that assign vectors to points in space. We will be discussing ◦ Line integrals—which can be used to find the work done by a force field in moving an object along a curve. ◦ Surface integrals—which can be used to find the rate of fluid flow across a surface. 16.1 Vector Fields2Dr. Erickson

3 Connections The connections between these new types of integrals and the single, double, and triple integrals we have already met are given by the higher-dimensional versions of the Fundamental Theorem of Calculus: ◦ Green’s Theorem ◦ Stokes’ Theorem ◦ Divergence Theorem 16.1 Vector Fields3Dr. Erickson

4 Velocity Vector Fields Some examples of velocity vector fields are: ◦ Air currents ◦ Ocean currents ◦ Flow past an airfoil 16.1 Vector Fields4Dr. Erickson

5 Force Field Another type of vector field, called a force field, associates a force vector with each point in a region. 16.1 Vector Fields5Dr. Erickson

6 Definition – Vector field on  2 Let D be a set in  2 (a plane region). A vector field on  2 is a function F that assigns to each point (x, y) in D a two-dimensional (2-D) vector F(x, y). 16.1 Vector Fields6Dr. Erickson

7 Vector Fields on  2 Since F(x, y) is a 2-D vector, we can write it in terms of its component functions P and Q as: F(x, y) = P(x, y) i + Q(x, y) j = or, for short, F = P i + Q j 16.1 Vector Fields7Dr. Erickson

8 Definition - Vector Field on  3 Let E be a subset of  3. A vector field on  3 is a function F that assigns to each point (x, y, z) in E a three-dimensional (3-D) vector F(x, y, z). 16.1 Vector Fields8Dr. Erickson

9 Velocity Fields Imagine a fluid flowing steadily along a pipe and let V(x, y, z) be the velocity vector at a point (x, y, z). ◦ Then, V assigns a vector to each point (x, y, z) in a certain domain E (the interior of the pipe). ◦ So, V is a vector field on  3 called a velocity field. 16.1 Vector Fields9Dr. Erickson

10 Velocity Fields A possible velocity field is illustrated here. ◦ The speed at any given point is indicated by the length of the arrow. 16.1 Vector Fields10Dr. Erickson

11 Gravitational Fields The gravitational force acting on the object at x = is: Note: Physicists often use the notation r instead of x for the position vector. So, you may see Formula 3 written in the form F = –(mMG/r 3 )r 16.1 Vector Fields11Dr. Erickson

12 Electric Fields Instead of considering the electric force F, physicists often consider the force per unit charge: ◦ Then, E is a vector field on  3 called the electric field of Q. 16.1 Vector Fields12Dr. Erickson

13 Example 1 Match the vector fields F with the plots labeled I-IV. Give reasons for your choices. 1. F(x, y) = 16.1 Vector Fields13Dr. Erickson

14 Example 2 – pg. 1086 # 34 At time t = 1, a particle is located at position (1, 3). If it moves in a velocity field find its approximate location at t = 1.05. 16.1 Vector Fields14Dr. Erickson


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