Physics 121: Electricity & Magnetism – Lecture 3 Electric Field

1. Physics 121: Electricity & Magnetism – Lecture 3Electric Field Dale E. Gary Wenda Cao NJIT Physics Department

2. What? -- Action on a distance How? – Electric Field Why? – Field Force Where? – in the space surrounding charges Electric Force and Field Force

3. Fields • Scalar Fields: • Temperature – T(r) • Pressure – P(r) • Potential energy – U(r) • Vector Fields: • Velocity field – • Gravitational field – • Electric field – • Magnetic field –

4. Vector Field Due to Gravity • When you consider the force of Earth’s gravity in space, it points everywhere in the direction of the center of the Earth. But remember that the strength is: • This is an example of an inverse-square force (proportional to the inverse square of the distance). m M

5. Idea of Test Mass • Notice that the actual amount of force depends on the mass, m: • It is convenient to ask what is the force per unit mass. The idea is to imagine putting a unit test mass near the Earth, and observe the effect on it: • g(r) is the “gravitational field.”

6. Electric Field • Electric field is said to exist in the region of space around a charged object: the source charge. • Concept of test charge: • Small and positive • Does not affect charge distribution • Electric field: • Existence of an electric field is a property of its source; • Presence of test charge is not necessary for the field to exist; + + + + + + + + +

7. Electric Field • A test charge of +3 µC is at a point P where an external electric field is directed to the right and has a magnitude of 4×106 N/C. If the test charge is replaced with another test charge of –3 µC, what happens to the external electric field at P? A. It is unaffected. B. It reverses direction. C. It changes in a way that cannot be determined.

8. Electric Field • Magnitude: E=F/q0 • Direction: is that of the force that acts on the positive test charge • SI unit: N/C

9. 2. Which diagram could be considered to show the correct electric force on a positive test charge due to a point charge? B. A. C. D. E.

10. Electric Field due to a Point Charge Q B A Q q0 • Direction is radial: outward for +|Q| inward for -|Q| • Magnitude: constant on any spherical shell • Flux through any shell enclosing Q is the same: EAAA = EBAB

11. Electric Field due to a group of individual charge

12. Example: Electric Field of a Dipole • Start with • If d << z, then, • So • E ~ 1/z3 • E =>0 as d =>0 • Valid for “far field”

13. Electric Field of a Continuous Charge Distribution • Find an expression for dq: • dq = λdl for a line distribution • dq = σdA for a surface distribution • dq = ρdV for a volume distribution • Represent field contributions at P due to point charges dq located in the distribution. Use symmetry, • Add up (integrate the contributions) over the whole distribution, varying the displacement as needed,

14. Example: Electric Field Due to a Charged Rod • A rod of length l has a uniform positive charge per unit length λ and a total charge Q. Calculate the electric field at a point P that is located along the long axis of the rod and a distance a from one end. • Start with • then, • So • Finalize • l => 0 ? • a >> l ?

15. Electric Field Lines • The electric field vector is tangent to the electric field line at each point. The line has a direction, indicated by an arrowhead, that is the same as that of the electric field vector. The direction of the line is that of the force on a positive test charge placed in the field. • The number of lines per unit area through a surface perpendicular to the lines is proportional to the magnitude of the electric field in that region. Thus, the field lines are close together where the electric field is strong and far apart where the field is weak.

16. Electric Field Lines • The lines must begin on a positive charge and terminate on a negative charge. In the case of an excess of one type of charge, some lines will begin or end infinitely far away. • The number of lines drawn leaving a positive charge or approaching a negative charge is proportional to the magnitude of the charge. • No two field lines can cross.

17. Electric Field .B 3. Rank the magnitudes E of the electric field at points A, B, and C shown in the figure. A) EC>EB>EA B) EB>EC>EA C) EA>EC>EB D) EB>EA>EC E) EA>EB>EC .C .A

18. Motion of a Charged Particle in a Uniform Electric Field • If the electric field E is uniform (magnitude and direction), the electric force F on the particle is constant. • If the particle has a positive charge, its acceleration a and electric force F are in the direction of the electric field E. • If the particle has a negative charge, its acceleration a and electric force F are in the direction opposite the electric field E.

19. A Dipole in an Electric Field • Start with • Then and • So

20. A Dipole in an Electric Field • Start with • Since • Choose at • So

21. 4. In which configuration, the potential energy of the dipole is the greatest? a c b E d e

22. Summary • Electric field E at any point is defined in terms of the electric force F that acts on a small positive test charge placed at that point divided by the magnitude q0 of the test charge: • Electric field lines provide a means for visualizing the direction and magnitude of electric fields. The electric field vector at any point is tangent to a field line through that point. The density of field lines in any region is proportional to the magnitude of the electric field in that region. • Field lines originate on positive charge and terminate on negative charge. • Field due to a point charge: The direction is away from the point charge if the charge is positive and toward it if the charge is negative. • Field due to an electric dipole: • Field due to a continuous charge distribution: treat charge elements as point charges and then summing via inegration, the electric field vectors produced by all the charge elements. • Force on a point charge in an electric field: • Dipole in an electric field: • The field exerts a torque on the dipole • The dipole has a potential energy U associated with its orientation in the field