'Infinite time' presentation slideshows

Perturbations around Black Hole solutions

Perturbations around Black Hole solutions. Elcio Abdalla. Classical (non-relativistic) Black Hole. The escape velocity is equal to the velocity of light Therefore,. The Schwarzschild Black Hole. Birckhoff Theorem: a static spherically Symmetric solution must be of the form

731 views • 57 slides

HAMILTON Software VENUS two

HAMILTON Software VENUS two. VENUS two General Steps. HAMILTON Software VENUS two. What are the General Steps?. The General Step group contains steps for multiple basic programming purposes.

1.41k views • 49 slides

Continuation of global bifurcations using collocation technique

Continuation of global bifurcations using collocation technique. In cooperation with: Bob Kooi, Yuri Kuznetsov (UU), Bas Kooijman. George van Voorn 3 th March 2006 Schoorl. Overview. Recent biological experimental examples of: Local bifurcations (Hopf) Chaotic behaviour

579 views • 37 slides

2012. 09 Takashi Suzuki

Exclusion of boundary blowup for 2D chemotaxis system with Dirichlet boundary condition for the Poisson part. 2012. 09 Takashi Suzuki. TexPoint fonts used in EMF. Read the TexPoint manual before you delete this box.: A A. The model. 1. Smoluchowski Part. other Poisson parts.

470 views • 34 slides

Chapter 2

Huseyin Bilgekul Eeng360 Communication Systems I Department of Electrical and Electronic Engineering Eastern Mediterranean University. Chapter 2. SIGNALS AND SPECTRA Chapter Objectives: Basic signal properties (DC, RMS, dBm, and power); Fourier transform and spectra;

388 views • 19 slides

Wave Packets

Wave Packets. Recall that for a wave packet ?x ?k~1 to localize a wave to some region ?x we need a spread of wavenumbers ?k de Broglie hypothesis ? =h/p or p=h/ ? but k=2?/? and p=(h/2?)(2?/?) = ? k h bar ?p= ? ?k and ?x ?p~ ? ?x ?p ? ? uncertainty principle.

1.21k views • 15 slides

Verbs: The Infinitive Construct

297 views • 13 slides

226 views • 12 slides

Energy

Energy. Conservative system E = T + V ( q ) Solve for the velocity. Position can be found analytically for some V ( q ). General solution is numeric. Oscillator in One Coordinate. Potential Energy. Turning points q 1 , q 2 v q = 0 V ( q 1 ) = V( q 2 ) = E

181 views • 9 slides