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Physics of Astronomy week 8 Thus. 25 May 2006 Crisis in Cosmology Planck Time Candidate solutions Looking ahead.

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Presentation on theme: "Physics of Astronomy week 8 Thus. 25 May 2006 Crisis in Cosmology Planck Time Candidate solutions Looking ahead."— Presentation transcript:

1 Physics of Astronomy week 8 Thus. 25 May 2006 Crisis in Cosmology Planck Time Candidate solutions Looking ahead

2 Astrophysics in crisis Black holes: what do you know? Big Bang: You’ve heard that “the laws of physics break down” in the earliest moment. Black holes can help us understand what that means.

3 Evidence for the Big Bang The 3-degree background radiation reveals the origin of structure in the universe

4 More evidence for the Big Bang Expansion of the universe: further galaxies are receding faster Primordial abundances of Hydrogen, Helium and metals 3K radiation: universe has cooled to the present Inflation: solution of horizon and flatness problems

5 Questions about the Big Bang What happened in the first tenth of a millionth of a billionth of a billionth of a billionth of a billionth of a second (10 -43 sec)? The universe was very small, so ask Quantum Mechanics. The universe was very massive and dense, so ask General Relativity (theory of gravity).

6 Current paradigms in physics Quantum Mechanics explains the very small General Relativity explains the very massive (theory of gravity) http://fusionanomaly.net/quantummechanics.html http://www.phys.lsu.edu/dept/gifs/quantum.gif

7 How big was the universe in the beginning? R

8 General Relativity (gravity) The early universe was a singularity – mathematically like a black hole. Event horizon R = distance inside which everything (including light) is contained BH R

9 Quantum Mechanics The early universe was very small – a point. Small quantum objects have an uncertain size  R or wavelength  R=

10 Problem: the early singularity could be outside its own event horizon?! “Laws of physics break down” R  R=

11 Calculating the Planck scales: 1.Use energy conservation to find the GRAVITATIONAL size of a black hole, the Schwartzschild radius R. 2.Next, use the energy of light to calculate the QUANTUM MECH. size of a black hole, De Broglie wavelength. 3. Then, equate the QM size with the Gravitational size to find the PLANCK MASS M p of the smallest sensible black hole. 4. Finally, substitute M into R to find PLANCK LENGTH L p 5.and then calculate both M p and L p, and the Planck time. 6.These are the smallest scales that we can describe with both GR and QM. At smaller scales, GR and QM are mutually inconsistent.

12 1a. Gravitational size of a Black Hole We can use energy conservation to find the size of a black hole. First, find the escape velocity (v) from an object with mass M and radius R: K initial + U initial = K final + U final ½ mv 2 – GmM/R = 0 + 0 Solve for v: MRMR mv m v→0, r→0

13 1b. Gravitational size of a Black Hole For a black hole with mass M, the escape velocity v=c at the event horizon r = R grav = Schwartzschild radius BH R

14 2. Quantum mechanical size of a Black Hole The deBroglie wavelength,, describes the smallest region of space in which a particle (or a black hole) of mass m can be localized, according to quantum mechanics.

15 3. Find the Planck mass, M p If a black hole had a mass less than the Planck mass M p, its quantum-mechanical size could be outside its event horizon. This wouldn’t make sense, so M p is the smallest possible black hole.

16 4. Find the Planck length, L p These both yield the Planck length, L p. Any black hole smaller than this could have its singularity outside its event horizon. That wouldn’t make sense, so L is the smallest possible black hole we can describe with both QM and GR, our current theory of gravity.

17 5. Calculate the Planck length and mass These are smallest scales we can describe with both QM and GR.

18 6. Calculate the Planck time Consider the time it would take for light to cross the Planck length: Speed = distance / time c = L p /  p Solve for the Planck time  p :

19 Planck scales You should find roughly these sizes for the: Planck mass = ~ 3 x 10 -8 kg ~ 4 x 10 -35 m (A black hole smaller than this could be outside its own event horizon, so QM and gravity are not both consistent at this scale.) ~ 10 -43 s (At earlier times, our familiar laws of physics “break down”.)

20 Outstanding cosmological questions What physics operated before the Planck time? What is gravity? Higgs? Graviton? Other? What is dark matter? Neutrinos? Wimps? What is dark energy? Why does universe’s expansion accelerate? How to unite gravity with QM? Loop quantum gravity? Superstrings? D-branes? Supersymmetric particles?

21 We need a new theory of “quantum gravity” String theory? Loop quantum gravity? http://www.columbia.edu/cu/record/archives/vol23/vol23_iss18/28c.gifhttp://www.columbia.edu/cu/record/archives/vol23/vol23_iss18/28c.gif http://www.cpt.univ-mrs.fr/~rovelli/rovelli.html Will one of these resolve the crisis and become our ultimate GUT?

22 How to choose which model? Criteria: * New model answers old Q * Predictions pass tests * New puzzles solvable * Simplicity, beauty * More? My generation articulated this problem. Your generation will solve it.

23 Looking ahead Research posters tomorrow at Science Carnival Research reports Tuesday Summative lecture Tuesday Final Thursday

24 Research reports Approx. 5 pages – concise and clear + annotated bibliography + appendices: calculations and figures + reference sources at end of each sentence! TEAMS: make it clear what each team member contributed, to the work and to the writing Each team member should demonstrate his or her understanding INDEPENDENTLY MAKE IT YOUR OWN – unique and original


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