1. Chapter 21 Electric Field and Coulomb’s Law (again) Coulomb’s Law (sec. 21.3) Electric fields & forces (sec. 21.4 & -6) Vector addition C 2009 J. F. Becker

2. Vectors (Review) Used extensively throughout the course INTRODUCTION: see Ch. 1 (Volume 1) C 2009 J. Becker

3. Vectors are quantities that have both magnitude and direction. An example of a vector quantity is velocity. A velocity has both magnitude (speed) and direction, say 60 miles per hour in a DIRECTION due west. (A scalar quantity is different; it has only magnitude – mass, time, temperature, etc.)

4. A vector may be composed of its x- and y- components as shown.

5. Note: The dot product of two vectors is a scalar quantity. The scalar (or dot) product of two vectors is defined as C 2009 J. F. Becker

6. The vector (or cross) product of two vectors is a vector where the direction of the vector product is given by the right-hand rule. The MAGNITUDE of the vector product is given by: C 2009 J. F. Becker Note: The dot product of two vectors is a scalar quantity.

7. Right-hand rule for DIRECTION of vector cross product.

8. Coulomb’s Law Coulomb’s Law lets us calculate the FORCE between two ELECTRIC CHARGES.

9. Coulomb’s Law Coulomb’s Law lets us calculate the force between MANY charges. We calculate the forces one at a time and ADD them AS VECTORS. (This is called “superposition.”) THE FORCE ON q 3 CAUSED BY q 1 AND q 2.

10. 21-9 Coulomb’s Law – vector problem Net force on charge Q is the vector sum of the forces by the other two charges. Coulomb’s Law -forces between two charges

11. Recall GRAVITATIONAL FIELD near Earth: F = G m 1 m 2 /r 2 = m 1 (G m 2 /r 2 ) = m 1 g where the vector g = 9.8 m/s 2 in the downward direction, and F = m g. ELECTRIC FIELD is obtained in a similar way: F = k q 1 q 2 /r 2 = q 1 (k q 2 /r 2 ) = q 1 (E) where the vector E is the electric field caused by q 2. The direction of the E field is determined by the direction of the F, or as you noticed in lab #1, the E field lines are directed away from a positive q 2 and toward a -q 2. The F on a charge q in an E field is F = q E and |E| = (k q 2 /r 2 ) C 2009 J. F. Becker

12. A charged body creates an electric field. Coulomb force of repulsion between two charged bodies at A and B, (having charges Q and q o respectively) has magnitude: F = k |Q q o |/r 2 = q o [ k Q/r 2 ] where we have factored out the small charge q o. We can write the force in terms of an electric field E: Therefore we can write for F = q o E the electric field E = [ k Q / r 2 ]

13. Calculate E 1, E 2, and E TOTAL at points “A” & “C”: q = 12 nC Electric field at“A” and “C” set up by charges q 1 and q 1 (an electric dipole) a) E 1 = 3.0 (10) 4 N/C E 2 = 6.8 (10) 4 N/C E A = 9.8 (10) 4 N/C c) E 1 = 6.4 (10) 3 N/C E 2 = 6.4 (10) 3 N/C E C = 4.9 (10) 3 N/C in the +x-direction A C Lab #1

14. Electric field at P caused by a line of charge along the y-axis. Consider symmetry! E y = 0 XoXo y

15. XoXo dq o dE x = dE cos a =[k dq /x o 2 +a 2 ][x o /(x o 2 + a 2 ) 1/2 ] E x = k x o  dq /[x o 2 + a 2 ] 3/2 where x o is constant as we add all the dq’s (=Q) in the integration: E x = k x o Q/[x o 2 +a 2 ] 3/2 |dE| = k dq / r 2 cos a =x o / r

16. Calculate the electric field at +q caused by the distributed charge +Q. Tabulated integral :  dz / (c-z) 2 = 1 / (c- z) d b

17. Electric field at P caused by a line of charge along the y-axis. Consider symmetry! E y = 0 XoXo y

18. Electric field at P caused by a line of charge along the y-axis. Consider symmetry! E y = 0 XoXo y Tabulated integral :  dz / (c 2 +z 2 ) 3/2 = z / c 2 (c 2 +z 2 ) 1/2

19. Tabulated integral : (Integration variable “z”)  dz / (c 2 +z 2 ) 3/2 = z / c 2 (c 2 +z 2 ) 1/2  dy / (c 2 +y 2 ) 3/2 = y / c 2 (c 2 +y 2 ) 1/2  dy / ( X o 2 +y 2 ) 3/2 = y / X o 2 ( X o 2 +y 2 ) 1/2 Our integral=k (Q/2a) X o 2 [ y / X o 2 ( X o 2 +y 2 ) 1/2 ] 0 a E x = k (Q /2a) X o 2 [( a –0) / X o 2 ( X o 2 +a 2 ) 1/2 ] E x = k (Q /2a) X o 2 [ a / X o 2 ( X o 2 +a 2 ) 1/2 ] E x = k (Q / X o ) [ 1 / ( X o 2 +a 2 ) 1/2 ] Notation change C 2009 J. F. Becker

20. Calculate the electric field at -q caused by +Q, and then the force on -q. Tabulated integral:  dz / (z 2 + a 2 ) 3/2 = z / a 2 (z 2 + a 2 ) 1/2  z dz / (z 2 + a 2 ) 3/2 = -1 / (z 2 + a 2 ) 1/2

21. An ELECTRIC DIPOLE consists of a +q and –q separated by a distance d. ELECTRIC DIPOLE MOMENT is p = q d ELECTRIC DIPOLE in E experiences a torque:  = p x E ELECTRIC DIPOLE in E has potential energy: U = - p E C 2009 J. F. Becker

22. Net force on an ELECTRIC DIPOLE is zero, but torque (  ) is into the page.  = r x F  = p x E ELECTRIC DIPOLE MOMENT is p = qd

23. See www.physics.edu/becker/physics51 Review C 2009 J. F. Becker