Portfolios Wiki courses:lecture:cflec http://sites.science.oregonstate.edu/portfolioswiki/ 2020-01-27T00:57:09-08:00 Portfolios Wiki http://sites.science.oregonstate.edu/portfolioswiki/ http://sites.science.oregonstate.edu/portfolioswiki/lib/images/favicon.ico text/html 2011-08-16T17:46:42-08:00 courses:lecture:cflec:cflecangularmomentum http://sites.science.oregonstate.edu/portfolioswiki/courses:lecture:cflec:cflecangularmomentum?rev=1313542002 Introduction to Angular Momentum Lecture ( minutes) [Central Forces Notes] Section 6 text/html 2011-08-16T17:46:42-08:00 courses:lecture:cflec:cflecassoclegpoly http://sites.science.oregonstate.edu/portfolioswiki/courses:lecture:cflec:cflecassoclegpoly?rev=1313542002 Associated Legendre Polynomials Lecture (20 minutes) [Central Forces Notes] Section 25 text/html 2013-04-11T17:02:52-08:00 courses:lecture:cflec:cfleccenterofmass http://sites.science.oregonstate.edu/portfolioswiki/courses:lecture:cflec:cfleccenterofmass?rev=1365724972 Derivation and Explanation of Center of Mass Lecture (15 minutes) [Central Forces Notes] Section 3 --Survivor Outerspace Activity. text/html 2013-04-05T11:31:28-08:00 courses:lecture:cflec:cfleccentralforce http://sites.science.oregonstate.edu/portfolioswiki/courses:lecture:cflec:cfleccentralforce?rev=1365186688 Definition of a Central Force Lecture [Central Forces Notes] Section 5 central text/html 2013-04-05T11:23:47-08:00 courses:lecture:cflec:cfleccfmotionassumptions http://sites.science.oregonstate.edu/portfolioswiki/courses:lecture:cflec:cfleccfmotionassumptions?rev=1365186227 Interactive Lecture on Assumptions about Central Force Motion ( minutes) [Central Forces Notes] Section 5 $$m_1\dfrac{d^2}{dt^2}\vec{r}_1=\vec{F}_{1,ext}-\vec{f}_{12}$$ $$m_2\dfrac{d^2}{dt^2}\vec{r}_2=\vec{F}_{2,ext}+\vec{f}_{12}$$ text/html 2011-08-16T17:49:51-08:00 courses:lecture:cflec:cflecclassicallim http://sites.science.oregonstate.edu/portfolioswiki/courses:lecture:cflec:cflecclassicallim?rev=1313542191 The Classical Limit Lecture ( minutes) [Hydrogen orbitals for large and small values of m] text/html 2011-08-16T17:46:42-08:00 courses:lecture:cflec:cfleceffpotential http://sites.science.oregonstate.edu/portfolioswiki/courses:lecture:cflec:cfleceffpotential?rev=1313542002 Energy and Effective Potential Lecture (25 minutes) [Central Forces Notes] Sections 11 and 12 small whiteboard question text/html 2011-07-04T15:42:01-08:00 courses:lecture:cflec:cflechydrogencalculations http://sites.science.oregonstate.edu/portfolioswiki/courses:lecture:cflec:cflechydrogencalculations?rev=1309819321 Quantum Calculations on the Hydrogen Atom Lecture (60 minutes) $$P(-3 \hbar) = \sum^{\infty}_{n=4} \sum^{n-1}_{l=3} |\langle n, l, m| \Psi \rangle |^2$$ text/html 2011-08-16T17:46:42-08:00 courses:lecture:cflec:cflechydrogenradialeq http://sites.science.oregonstate.edu/portfolioswiki/courses:lecture:cflec:cflechydrogenradialeq?rev=1313542002 Solving the Radial Equation Lecture (45 minutes) [Central Forces Notes] Section 28-30 text/html 2011-08-16T17:46:42-08:00 courses:lecture:cflec:cflechydrogensols http://sites.science.oregonstate.edu/portfolioswiki/courses:lecture:cflec:cflechydrogensols?rev=1313542002 Lecture ( minutes) [Central Forces Notes] Section 31 $${R_n}^\ell (r){Y_\ell }^m\left( \theta ,\phi \right) = \sqrt { { {\left( {\frac{2}{{n{a_0} } } } \right)}^3}\frac{{\left( {n - \ell - 1} \right)!} }{{2n{ {\left( {\left( {n + \ell } \right)!} \right)}^3} } } } {\left( {\frac{{2r} }{{n{a_0} } } } \right)^\ell }{e^{ - \frac{r}{ {n{a_0} } } } }L_{n + \ell }^{2\ell + 1}\left( {\frac{ {2r} }{ {n{a_0} } } } \right){Y_\ell }^m\left( {\theta ,\phi } \right)$$ text/html 2018-03-16T11:02:08-08:00 courses:lecture:cflec:cfleclegprops http://sites.science.oregonstate.edu/portfolioswiki/courses:lecture:cflec:cfleclegprops?rev=1521223328 Lecture (10 minutes) text/html 2011-08-16T17:46:42-08:00 courses:lecture:cflec:cfleclegseries http://sites.science.oregonstate.edu/portfolioswiki/courses:lecture:cflec:cfleclegseries?rev=1313542002 Legendre Series Lecture (20 minutes) [Central Forces Notes] Section 24 $$a_k = (k + \frac{1}{2})\int_{-1}^1 P_k(z)^* f(z) dz $$ Small Whiteboard Questions Students often struggle with this, but it is helpful to remind them of the way you find coefficients for a vector (by taking the dot product,, and coefficients for a Fourier series (the inner product for functions, Common Student Questions “” text/html 2012-03-14T14:18:40-08:00 courses:lecture:cflec:cflecloperators http://sites.science.oregonstate.edu/portfolioswiki/courses:lecture:cflec:cflecloperators?rev=1331759920 Spherical Harmonics and the $H$, $L^2$, and $L_z$ Operators Lecture (60 minutes) [Central Forces Notes] Section 27 text/html 2013-04-11T16:59:26-08:00 courses:lecture:cflec:cflecorbitshape http://sites.science.oregonstate.edu/portfolioswiki/courses:lecture:cflec:cflecorbitshape?rev=1365724766 Finding the Shape of the Orbit (Kepler's 1st Law) Lecture (25 minutes) [Central Forces Notes] Section 10 text/html 2016-07-11T13:45:05-08:00 courses:lecture:cflec:cflecpolar http://sites.science.oregonstate.edu/portfolioswiki/courses:lecture:cflec:cflecpolar?rev=1468269905 Kepler's 2nd Law in Polar Coordinates Lecture (5 minutes) [Central Forces Notes] Section 8 Velocity and Acceleration in Polar Coordinates \begin{align*} \vec{L}&=\vec{r}\times\vec{p}\\ &=\vec{r}\times\mu\vec{v}\\ &=r\hat{r}\times\mu\left(\dot{r}\hat{r}+r\dot{\phi}\hat{\phi}\right)\\ &=\mu r^2\dot{\phi}\;\hat{r}\times\hat{\phi}\\ &=\mu r^2\dot{\phi}\hat{z}\text{ (cylindrical)}\\ &=-\mu r^2\dot{\phi}\hat{\theta}\text{ (spherical)} \end{align*} text/html 2013-04-11T16:56:07-08:00 courses:lecture:cflec:cflecpositionvec http://sites.science.oregonstate.edu/portfolioswiki/courses:lecture:cflec:cflecpositionvec?rev=1365724567 Position Vector Lecture/Discussion (15 minutes) [Central Forces Notes] Section 7 text/html 2011-07-04T15:41:01-08:00 courses:lecture:cflec:cflecpostulatesofqm http://sites.science.oregonstate.edu/portfolioswiki/courses:lecture:cflec:cflecpostulatesofqm?rev=1309819261 Postulates of Quantum Mechanics Note: A common misconception among students first learning quantum mechanics is that a measurement is carried out by operating on a ket with the operator associated with observable one wants to measure. text/html 2011-08-16T17:46:42-08:00 courses:lecture:cflec:cflecradialeq http://sites.science.oregonstate.edu/portfolioswiki/courses:lecture:cflec:cflecradialeq?rev=1313542002 Finding the Radial Equation from Conservation of Energy Lecture (15 minutes) [Central Forces Notes] Section 11 text/html 2011-08-16T17:46:42-08:00 courses:lecture:cflec:cflecreducedmass http://sites.science.oregonstate.edu/portfolioswiki/courses:lecture:cflec:cflecreducedmass?rev=1313542002 Derivation of Reduced Mass Lecture [Central Forces Notes] Section 4 $${{m_1 m_2}\over {m_1+m_2}} {d{^2}\over{d{t^2}}} (\Vec{r_1}-\Vec{r_2}) = \Vec{f_{12}}$$ text/html 2011-08-16T17:46:42-08:00 courses:lecture:cflec:cflecreducedmasshamiltonian http://sites.science.oregonstate.edu/portfolioswiki/courses:lecture:cflec:cflecreducedmasshamiltonian?rev=1313542002 Lecture on the Derivation of the Hamiltonian in terms of Reduced Mass (20 minutes) [Central Forces Notes] Section 14. text/html 2011-08-16T17:46:42-08:00 courses:lecture:cflec:cflecreviewhamiltonian http://sites.science.oregonstate.edu/portfolioswiki/courses:lecture:cflec:cflecreviewhamiltonian?rev=1313542002 Review of Hamiltonians Lecture (20 minutes) [Central Forces Notes] Section 13 This lecture reviews what students have learned about Schrödinger's equation and the Hamiltonian from previous classes. small whiteboard question $$\hat{H}= \frac{\hbar^2}{2 m_p} \nabla^2_p + \frac{\hbar^2}{2 m_e} \nabla^2_e -\frac{1}{4 \pi \epsilon_0} \frac{e^2}{|r_p-r_e|}$$ where $$\nabla^2_p = \frac{1}{r_p^2} \frac{\partial}{\partial r_p} \left(r_p^2 \frac{\partial}{\partial r_p} \right)+ \frac{1}{r_p^2 \sin(\t… text/html 2011-08-16T17:46:42-08:00 courses:lecture:cflec:cflecringangmomentum http://sites.science.oregonstate.edu/portfolioswiki/courses:lecture:cflec:cflecringangmomentum?rev=1313542002 Angular Momentum on the Ring Lecture (20 minutes) [Central Forces Notes] Section 18 text/html 2011-08-16T17:46:42-08:00 courses:lecture:cflec:cflecringeigenstates http://sites.science.oregonstate.edu/portfolioswiki/courses:lecture:cflec:cflecringeigenstates?rev=1313542002 Finding the Eigenstates for the Ring Lecture (30 minutes) [Central Forces Notes] Section 17 small whiteboard question text/html 2011-08-16T17:46:42-08:00 courses:lecture:cflec:cflecsepofvariables http://sites.science.oregonstate.edu/portfolioswiki/courses:lecture:cflec:cflecsepofvariables?rev=1313542002 Separation of Variables in Spherical Coordinates Lecture (30 minutes) [Central Forces Notes] Section 33 (Appendix B) and 16 text/html 2012-08-09T15:48:24-08:00 courses:lecture:cflec:cflecseriessoltheta http://sites.science.oregonstate.edu/portfolioswiki/courses:lecture:cflec:cflecseriessoltheta?rev=1344552504 Solving the $\Theta$ Equation using the Series Solution Method (90 minutes) FIXME See 2012 video for series solution lecture with sequence of SWBQs. [Central Forces Notes] Section 20-23 Small White Board Questions Students sometimes have difficulty with this the first time they do it because they are not used to using the recurrence relation in this way. In addition, they do not realize that they need to set the values of $a_0$ and $a_1$. Common Student Confusions/Questions text/html 2013-04-11T15:39:52-08:00 courses:lecture:cflec:cflecsolveeqofmotion http://sites.science.oregonstate.edu/portfolioswiki/courses:lecture:cflec:cflecsolveeqofmotion?rev=1365719992 Solution to the Central Force Equation of Motion in Polar Coordinates Lecture (30 minutes) [Central Forces Notes] Section 9 $$\mathbf{\hat{r}}:\; f(r)=\mu(\ddot{r}-r\dot{\phi}^2)$$ $$\mathbf{\hat{\phi}}:\;0=\mu(r\ddot{\phi}+2\dot{r}\dot{\phi})$$ text/html 2013-05-14T13:34:08-08:00 courses:lecture:cflec:cflecsphereharmonics http://sites.science.oregonstate.edu/portfolioswiki/courses:lecture:cflec:cflecsphereharmonics?rev=1368563648 Spherical Harmonics, the Solutions to the Rigid Rotor Lecture (30 minutes) [Central Forces Notes] Section 26 One analogy that seems to resonate with students, especially the musicians is that spherical harmonics are essentially the harmonics for a spherical drum. text/html 2011-08-16T17:45:29-08:00 courses:lecture:cflec:cflecylmcombo http://sites.science.oregonstate.edu/portfolioswiki/courses:lecture:cflec:cflecylmcombo?rev=1313541929 Combinations of $Y_{l,m}(\theta,\phi)$ and the Spherical Harmonic Series ( minutes) [Central Forces Notes] Section 26 text/html 2018-03-16T10:55:10-08:00 courses:lecture:cflec:cfmblec2d http://sites.science.oregonstate.edu/portfolioswiki/courses:lecture:cflec:cfmblec2d?rev=1521222910 Lecture (25 minutes) --