Presentation is loading. Please wait.

Presentation is loading. Please wait.

Start EM Ch.5: Magnetostatics finish Modern Physics Ch.7: J=L+S Methods of Math. Physics, Thus. 24 Feb. 2011, E.J. Zita Magnetostatics: Lorentz Force and.

Similar presentations


Presentation on theme: "Start EM Ch.5: Magnetostatics finish Modern Physics Ch.7: J=L+S Methods of Math. Physics, Thus. 24 Feb. 2011, E.J. Zita Magnetostatics: Lorentz Force and."— Presentation transcript:

1 Start EM Ch.5: Magnetostatics finish Modern Physics Ch.7: J=L+S Methods of Math. Physics, Thus. 24 Feb. 2011, E.J. Zita Magnetostatics: Lorentz Force and Biot-Savart Law Divergence and Curl of B; Ampere’s Law Modern Physics Spin, Energy levels, Zeeman effect Fine structure, Bohr magneton, J=L+S

2 Ex.5.2: Cycloid motion: B=Bx, E=Ez, find particle motion if it starts from rest at the origin. 1. Draw. 2. Qualitative analysis. 3. Quantitative analysis.

3 Ex.5.4: (a) A current I is uniformly distributed over a wire of circular cross section with radius a. Find J.

4 Ex.5 (b) Suppose the current density in the wire is proportional to the distance from the axis: J=ks (for some constant k). Find the total current in the wire.

5

6 Finding field B from current I Biot Savart law in general (5.32, p.215) Ampere’s law, when symmetry permits (p.221) Draw Ampere’s law:

7 Apply Stokes’ Thm. to Magnetostatics

8 Using Ampere’s law 1.Draw, 2. Qualitative analysis, 3. Quantitative Find B for an infinite uniform surface current K=Kx over the xy plane. (I=dK/dlength)

9 Using Ampere’s law 1.Draw, 2. Qualitative analysis, 3. Quantitative Find B for a solenoid with n closely wound turns per unit length on a cylinder of radius R and carrying a steady current I.

10

11 We’ll finish Ch.5 next week. Choose some HW problems…

12 Continuing Modern Physics Ch.7: H atom in Wave mechanics Spin, Energy levels Zeeman effect Fine structure Bohr magneton J=L+S

13 H-atom wavefunctions ↔ electron probability distributions: l = angular momentum wavenumber Discussion: compare Bohr model to Schrödinger model for H atom.

14 m l denotes possible orientations of L and L z (l=2) Wave-mechanics L ≠ Bohr’s n 

15 Stern-Gerlach showed line splitting, even when l=0. l = 1, m=0,±1 ✓ l = 0, m=0, s= ±1/2 Normal Zeeman effect Anomalous Zeeman effect

16 Magnetic moments shift energies in B fields

17 Spin S and orbit L couple to total angular momentum J = L + S

18 Spin-orbit coupling: spin of e - in orbital magnetic field of p Fine-structure splitting (e.g. 21-cm line) (Interaction of nuclear spin with electron spin (in an atom) → Hyper-fine splitting)

19 Total J + external magnetic field → Zeeman effect

20

21

22 History of atomic models: Thomson discovered electron, invented plum-pudding model Rutherford observed nuclear scattering, invented orbital atom Bohr quantized angular momentum, improved H atom model. Bohr model explained observed H spectra, derived E n = E/n 2 and phenomenological Rydberg constant Quantum numbers n, l, m l (Zeeman effect) Solution to Schrödinger equation shows that E n = E/l(l+1) Pauli proposed spin (m s = ±1/2), and Dirac derived it Fine-structure splitting reveals spin quantum number


Download ppt "Start EM Ch.5: Magnetostatics finish Modern Physics Ch.7: J=L+S Methods of Math. Physics, Thus. 24 Feb. 2011, E.J. Zita Magnetostatics: Lorentz Force and."

Similar presentations


Ads by Google