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Sunday, January 25, 2015

Experiments with Lasers

I found this great video and made the translation.
I hope you can enjoy it.



You can found another cool experiments here:


CAUTION: Don't point a laser to your eyes. It's recommend an adult supervisor to all the experiments.

Wednesday, January 14, 2015

Chasing Comets

This is the first Inspiring Science Education Hangouts conducted by Dr. Pamela Gay:



This is part one of two. See the second part here: https://plus.google.com/events/coli5l...

"The solar system is littered with Ice. The bulk of this material orbits quietly in the outer Solar System, but sometimes, something disturbs the ice and the come plunging in toward the Sun. In this Hangout, we will discuss comets, how we explore them, and how they brought water to worlds like Earth."

The educational scenario can be found here: http://portal.opendiscoveryspace.eu/community/chasing-comets-774702?msg_id=23134

Friday, November 21, 2014

two new particles


"Today the collaboration for the LHCb experiment at CERN1’s Large Hadron Collider announced the discovery of two new particles in the baryon family. The particles, known as the Xi_b'- and Xi_b*-, were predicted to exist by the quark model but had never been seen before. A related particle, the Xi_b*0, was found by the CMS experiment at CERN in 2012. The LHCb collaboration submitted a paper reporting the finding to Physical Review Letters." Source: CERN

Read more:

Wednesday, November 12, 2014

Monday, November 10, 2014

Rosetta live online

Wednesday you can follow the online emission here: http://www.opendiscoveryspace.eu/news/rosetta-rendezuous-comet-697664
It will be a very important day, Philae will be landind on comet 67P/Churyumov–GerasimenkoThe lander is expected to achieve the first controlled touchdown on a comet nucleus. Its instruments should obtain the first images from a comet's surface and make the first in situ analysis to find out what it is made of.

Image credit: ESA



Monday, November 3, 2014

Quantum Numbers

Quantum numbers describe values of conserved quantities in the dynamics of a quantum system. In the case of quantum numbers of electrons, they can be defined as "The sets of numerical values which give acceptable solutions to theSchrödinger wave equation for the Hydrogen atom". Perhaps the most important aspect of quantum mechanics is thequantization of observable quantities, since quantum numbers are discrete sets of integers or half-integers, although they could approach infinity in some cases. This is distinguished from classical mechanics where the values can range continuously. Quantum numbers often describe specifically the energy levels of electrons in atoms, but other possibilities include angular momentumspin, etc. Any quantum system can have one or more quantum numbers; it is thus difficult to list all possible quantum numbers.
There are four quantum numbers which can describe the electron completely.
The principal quantum number (n) describes the electron shell, or energy level, of an atom. The value of n ranges from 1 to the shell containing the outermost electron of that atom.
The azimuthal quantum number () (also known as the angular quantum number or orbital quantum number) describes the subshell, and gives the magnitude of the orbital angular momentum.
The magnetic quantum number (m) describes the specific orbital (or "cloud") within that subshell, and yields the projection of the orbital angular momentum along a specified axis.
The spin projection quantum number (ms) describes the spin (intrinsic angular momentum) of the electron within that orbital, and gives the projection of the spin angular momentum S along the specified axis. An electron has spin s = ½, consequently ms will be ±½, corresponding with "spin" and "opposite spin." Each electron in any individual orbital must have different spins because of the Pauli exclusion principle, therefore an orbital never contains more than two electrons.
NameSymbolOrbital meaningRange of valuesValue examples
principal quantum numbernshell1 ≤ nn = 1, 2, 3, …
azimuthal quantum number (angular momentum)subshell (s orbital is listed as 0, p orbital as 1 etc.)0 ≤  ≤ n − 1for n = 3:
 = 0, 1, 2 (s, p, d)
magnetic quantum number, (projection ofangular momentum)menergy shift (orientation of the subshell's shape) ≤ m ≤ for  = 2:
m = −2, −1, 0, 1, 2
spin projection quantum numbermsspin of the electron (−½ = "spin down", ½ = "spin up")s ≤ ms ≤ sfor an electron s = ½,
so ms = −½, ½



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