8/25/2015 WHY TAKING THIS COURSE? MWF 9:30 – 10:20 MSB306 Lee Chow Department of Physics University of Central Florida Orlando, FL 32816 E&M is a well-established field. A complete theory is available. Through E&M, we can learn the approach to a problem from physicist’s point of view. Electricity & Magnetism I 8/20/2014 ELECTRICITY AND MAGNETISM I It is important. It can be applied to other fields. The concept of potential can be used in gravitational field. The field concept leads to QED, and the unification leads to the Grand Unification Theory and superstring theory. It is useful. Almost all the « Everyday » life experience of forces deal with E&M. 2 Chap. 2 Electrostatics What we will learn from E&M I ? • Curvilinear Coordinates ∭ · Gauss Law E field is conservative • Delta Function Electricity & Magnetism I • Integral Calculus E field due to charge density 8/20/2014 • Differential calculus Coulomb law (point charge) Electricity & Magnetism I • Vector algebra 8/20/2014 Chap. 1 Vector analysis and Integral Calculus ∮ · ℓ ⟹ Scalar potential 3 4 Poisson’s equation Chap. 3 Special Techniques Chap. 4 Electrostatic field in matter • Separation of Variables • Spherical Coordinates • Multiple Expansion • Surface charge (bound) σ • Volume charge (bound) • Electric displacement • 5 • Polarization Electricity & Magnetism I Electricity & Magnetism I • Image method 8/20/2014 8/20/2014 Mainly mathematics Relation between & · 6 1 8/25/2015 Chap 5 Magnetostatics Chap 6 Magnetic Field in Matter • Ampere’s law · • No magnetic monopole • Magnetization • The field of a magnetized object • The Auxiliary field H • Vector potential • Electricity & Magnetism I Electricity & Magnetism I ℓ • Biot-Savart law 8/20/2014 8/20/2014 • Lorentz force law • Linear and Nonlinear Media · (Gauge selection) • (Poisson’s Equation) 7 8 Review of 2049 ∮ · , • Electric Potential • Energy density in E field, • Ohm’s Law V=IR • Current and Resistance · • Potential • Dielectric materials, Electricity & Magnetism I Electricity & Magnetism I • Electric field • Parallel plate capacitor, 8/20/2014 8/20/2014 • Coulomb’s Law • Gauss Law , • Capacitance • Potential relation • Circuits (AC & DC) 9 10 Maxwell Equations · • Magnetic Flux · • Lorentz Force 11 • ∮ · · • ∮ · · • ∮ · • ∮ · Electricity & Magnetism I • Faraday’s Law Electricity & Magnetism I • Biot-Savart Law 8/20/2014 ∮ 8/20/2014 • Ampere’s Law 12 2 8/25/2015 Major Laws in E&M . · From divergence theorem, · · Electricity & Magnetism I Electricity & Magnetism I · Concept of the Field 8/20/2014 8/20/2014 1. Coulomb law 2. Gauss Law (Point charge) · (Charge distribution) (differential form) 13 Relationship between Coulomb law and Gauss law Gauss law is easier to solve when symmetry is involved. · · = · , measures the spread out of · In Cartesian Coordinates, · 15 4. Curl of the field. Therefore · is always true. 17 Since the curl of a gradient is always equal to zero ( , we can see from last equation that the electric field, can be expressed as a gradient of a scalar potential: This also implied that the is a conservative field, Electricity & Magnetism I 16 8/20/2014 The integral does not depend on the path Electricity & Magnetism I · 8/20/2014 In electrostatic, the curl of field is equal to zero. We can start with Coulomb law · Electricity & Magnetism I · The divergence of the electric field, field 8/20/2014 · Electricity & Magnetism I · 3. Divergence of 8/20/2014 Gauss law and Coulomb law are closely related. 14 18 3 8/25/2015 7. Continuity equation 5. Lorentz force law. (Magneto-statics) · 8. Ampere’s Law · Electricity & Magnetism I Electricity & Magnetism I 6. Biot-Savart Law is 8/20/2014 8/20/2014 There is no work done by the B field because perpendicular to . This is the magnetic analogy of Gauss Law. 19 20 9. Divergence of the B field 10. Curl of B From Ampere’s law, ∮ · · · Electricity & Magnetism I Because there is no magnetic monopole. 8/20/2014 · · 21 4