An equilibrium is finally reached when the potential difference is a few times the electron temperature.

The ion temperature must be much smaller than the electron temperature.

The electron temperature in the streamers only reaches 0.7 eV.

"Bremsstrahlung reading is way up, and electron temperature is dropping."

Even in a "cold" plasma, the electron temperature is still typically several thousand degrees Celsius.

The relatively low electron temperature makes probe construction straightforward and does not require the use of exotic materials.

A common rule of thumb for this voltage bias is 3 times the expected electron temperature in eV.

Often the electron temperature is handled separately from the temperature of the remaining gas components.

The electron temperature can be determined very reliably from the Doppler broadening of the laser line.

For this reason, the "ion temperature" may be very different from (usually lower than) the "electron temperature".

That is, the voltage difference between the positive and floating electrodes is proportional to the electron temperature.

In most plasmas of interest, the electron temperature is comparable to or larger than the ion temperature.

The radar reveals a number of poleward-moving regions in which the electron temperature is elevated by a factor of 1.5.

(It is usually a good assumption that the electron temperature will be nearly equal to the ion temperature.

Stable operation with several megawatts in power output had been experimentally achieved as from 1967 with high electron temperature.

Langmuir probes (for electron temperature of a plasma)

Without quantitative modeling of the bulk resistivity, Langmuir probes can only give an upper limit on the electron temperature.

Tis the electron temperature.

Nevertheless experimental studies about the growth rate of the electrothermal instability and the critical conditions showed that a stability region still exists for high electron temperatures.

Magnetospheric double layers typically have a strength (where the electron temperature is assumed to lie in the range () and are therefore weak.

One advantage of ultracold plasmas are their well characterized and tunable initial conditions, including their size and electron temperature.

At this conference, Soviet scientists announced that they had achieved electron temperatures of over 1000 eV in a tokamak device (T-3).

Because the electron has a mass and diameter much smaller than the ion, the Electron temperature can be several orders of magnitude different then the ions.

The analysis presented here indicates how the electron temperature, electron density, and plasma potential can be derived from the I-V characteristic.

The inverse process of electron cyclotron emission can be used as a diagnostic of the radial electron temperature profile.