Phys 0175 - Lecture 32

Phys 0175 - Lecture 32 - Lecture 32 (Apr. 6, 2009):...

Info iconThis preview shows pages 1–6. Sign up to view the full content.

View Full Document Right Arrow Icon

Info iconThis preview has intentionally blurred sections. Sign up to view the full version.

View Full DocumentRight Arrow Icon

Info iconThis preview has intentionally blurred sections. Sign up to view the full version.

View Full DocumentRight Arrow Icon

Info iconThis preview has intentionally blurred sections. Sign up to view the full version.

View Full DocumentRight Arrow Icon
This is the end of the preview. Sign up to access the rest of the document.

Unformatted text preview: Lecture 32 (Apr. 6, 2009): Maxwells Equations; Magnetism (Ch. 32): Gauss Law for magnetic fields Induced magnetic fields Displacement current Maxwells equations and em radiation Magnetism and electrons Magnetic materials Chapter 32: Maxwells Equations Gauss Law for Magnetic Fields All experimental evidence to date points to the fact that there are no magnetic monopoles ; the simplest magnetic structure that produces a magnetic field is a single current loop (a magnetic dipole). This fact can be described in terms of Gauss Law applied to magnetic fields: Recall Gauss Law for electric fields: enc q E dA = r r g B dA = r r g Induced Magnetic Fields: Faradays law of induction was expressed as Symmetry suggests the question: If a changing magnetic flux induces an electric field, will a changing electric flux induce a magnetic field? The answer is yes: Maxwells law of induction 0 0 E d B ds dt = r r g B d E ds dt = - r r g Consider a parallel-plate capacitor with circular plates. Assume that the charge on the capacitor plates increases at a constant rate by a constant current i in the connecting wires. It follows that the electric field in the space between the plates will also increase at a constant rate. Fig. (b) is a view of the right-hand plate in Fig. (a) from between the plates. The electric field points into the page. Consider the electric flux passing through a circular hoop of radius r that is smaller than the radius of the plates. According to Maxwells law of induction there must be an induced magnetic field around the loop. This has been observed experimentally. If one considers a loop of radius r that is greater than the radius of the plates, one finds that a magnetic field is induced around that loop as well. Once the capacitor plates are fully charged, the electric field remains constant and the induced magnetic field becomes zero. Displacement current: Combining Maxwells law of induction with Amperes Law yields the Ampere-Maxwell law : Define displacement current:...
View Full Document

Page1 / 18

Phys 0175 - Lecture 32 - Lecture 32 (Apr. 6, 2009):...

This preview shows document pages 1 - 6. Sign up to view the full document.

View Full Document Right Arrow Icon
Ask a homework question - tutors are online