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EEE 340Lecture 041 2-4.3 Spherical Coordinates. EEE 340Lecture 042 A vector in spherical coordinates The local base vectors from a right –handed system.

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Presentation on theme: "EEE 340Lecture 041 2-4.3 Spherical Coordinates. EEE 340Lecture 042 A vector in spherical coordinates The local base vectors from a right –handed system."— Presentation transcript:

1 EEE 340Lecture 041 2-4.3 Spherical Coordinates

2 EEE 340Lecture 042 A vector in spherical coordinates The local base vectors from a right –handed system

3 EEE 340Lecture 043 The differential length The differential areas are The differential volume

4 EEE 340Lecture 044 On many occasions the differential areas are vectors

5 EEE 340Lecture 045 Table 2-1 Basic Orthogonal Coordinates Cartesian Cylindrical Spherical

6 EEE 340Lecture 046 Cartesian coordinates and are vectors. is a scalar. Differential displacement Differential normal area Differential volume

7 EEE 340Lecture 047 The differential surface element may be defined as we need to remember only !

8 EEE 340Lecture 048 Cylindrical coordinates Differential volume Differential normal area Differential displacement

9 EEE 340Lecture 049 Coordinate transforms Example 2-11. Convert a vector in spherical coordinates (SPC) into the Cartesian coordinates (CRT). Solution. The general form of a vector in the CRT is We need In fact

10 EEE 340Lecture 0410 The other eight dot-products can be worked out. A faster and better way to represent the transformation is based on the del operator.

11 EEE 340Lecture 0411 Example 2-12 Sphare chell r a =2 cm r b =5 cm The charge density Find the total charge Q

12 EEE 340Lecture 0412 Solution:

13 EEE 340Lecture 0413 2-5 Integrals Containing Vector Functions.

14 EEE 340Lecture 0414 The line integral around a close path C is denoted as In the Cartesian coordinates (CRT)

15 EEE 340Lecture 0415 Example 2-13 a) along the straight line OP, where P(1,1,0) P(1,1,0) y x 0 P1P1 P2P2

16 EEE 340Lecture 0416 b). Along path OP 1 P Solution. Using (2-52) of cylindrical a).


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