Investigating Equal Energies in a Plasma of 3 Populations

  • Thread starter Thread starter Heimdall
  • Start date Start date
  • Tags Tags
    Energies Plasma
Heimdall
Messages
38
Reaction score
0
Hi,

Let's consider a plasma of 3 distinct populations : 1 cold proton population of 0.2 density, 1 hot proton population of 0.8 density, and one electron population.

I have T_i=T_e and I set the velocity of my cold population to 0. I expected that te energy of my hot proton population to be equal to the energy of my electron population, but in fact the electrons are always a bit mor energetic than my protons.

Am I right, should I expect the energies to be equal ?
 
Physics news on Phys.org
Having distinct cold and hot populations of protons would be rather impossible - there is usually continuous distribution. The electrons would rapidly equilibrate to the proton temperatures since the electrons are much lighter and the coulomb forces are considerable. The electrons temperatures are approximately those of the protons for those reasons, and perhaps slightly cooler since electrons lose energy more readily due to brehmsstrahlung, and if magnetically confined, cyclotron radiation.

Only with external heating (e.g. RF) would electrons be hotter - but only while the external heating is applied.
 
Toponium is a hadron which is the bound state of a valance top quark and a valance antitop quark. Oversimplified presentations often state that top quarks don't form hadrons, because they decay to bottom quarks extremely rapidly after they are created, leaving no time to form a hadron. And, the vast majority of the time, this is true. But, the lifetime of a top quark is only an average lifetime. Sometimes it decays faster and sometimes it decays slower. In the highly improbable case that...
I'm following this paper by Kitaev on SL(2,R) representations and I'm having a problem in the normalization of the continuous eigenfunctions (eqs. (67)-(70)), which satisfy \langle f_s | f_{s'} \rangle = \int_{0}^{1} \frac{2}{(1-u)^2} f_s(u)^* f_{s'}(u) \, du. \tag{67} The singular contribution of the integral arises at the endpoint u=1 of the integral, and in the limit u \to 1, the function f_s(u) takes on the form f_s(u) \approx a_s (1-u)^{1/2 + i s} + a_s^* (1-u)^{1/2 - i s}. \tag{70}...
Back
Top