Energy production from deuterium plasma?

malagrond
Messages
2
Reaction score
0
First off, I would like to apologize for my ignorance. I am a college freshman, computer science, so I'm not as educated as I would like in the areas of physics that interest me most. On to my question, though.

I'm wondering if someone could provide an equation describing the energy released by deuterium plasma at given amount, temperature, and pressure, with the temperature and pressure being constant. Assume the system is self-sufficient such that no continuous input is required. Also, in what form would this energy be released?

Any help is greatly appreciated.

~Mala
 
Physics news on Phys.org
malagrond said:
First off, I would like to apologize for my ignorance. I am a college freshman, computer science, so I'm not as educated as I would like in the areas of physics that interest me most. On to my question, though.

I'm wondering if someone could provide an equation describing the energy released by deuterium plasma at given amount, temperature, and pressure, with the temperature and pressure being constant. Assume the system is self-sufficient such that no continuous input is required. Also, in what form would this energy be released?

Any help is greatly appreciated.

~Mala
One is interested in the fusion energy produced in a plasma? Typically that is given by Q * RR, where Q is the energy per reaction and RR is the reaction rate, which is given by n2/2 <σv>, where n is the deuteron density, and <σv> is the reaction rate parameter, which is a function of plasma temperature.

The energy from fusion is released as kinetic energy of the products, but these products interact with the electrons and other nuclei to heat the plasma. At the same time, electrons lose energy through brehmstrahlung and cyclotron radiation. Neutral atoms can also leak from the plasma.
 
Sorry for the delayed reply. Thank you very much for your help; I've made significant progress. Just to double-check my work, however, what units should I end up with?

~Mala
 
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}...

Similar threads

Back
Top