Frequency on the incident GNE-371 Epigenetic Reader Domain microwave is higher than the electron plasma
Frequency from the incident microwave is greater than the electron plasma frequency, the interaction from the would be with person electrons is reasonably to the incident inertia of an electronmicrowave as well high to allow it to respond fullyinsignificant. Therefore, distinctive Thus, the interaction in the microwave with individual by controlling microwave. interaction modes of microwaves with electrons could be achievedelectrons is the frequencies of the second incident microwaves [27]. reasonably insignificant. Thus, distinct interaction modes of microwaves with electrons The electron plasma frequency is really a function on the electron quantity density and is is usually achieved by controlling the frequencies of your second incident microwaves [27]. provided by [27]. The electron plasma frequency can be a function of your electron number density and is n e e2 offered by [27]. pe = 2v pe = (1) (rad/s) 0 me (1) pe = two = / exactly where pe is definitely the electron number density in Hz. The ne will be the electron density, the 0 could be the permittivity of absolutely free space, as well as the me could be the mass of an electron. As outlined by Equation (1), where is definitely the electron -3 number density in Hz. The would be the electron density, the is for ne = 1.56 1016 m , the electron plasma frequency is e = 1123 MH, that is situated the permittivity of absolutely free space, and the will be the mass of an electron. In accordance with between 2450 MHz and 915 MHz. Then, if the input microwave from Port 2 is 2450 or Equation (1), for = 1.56 ten , the electron plasma frequency is = 1123 MH, 915 MHz, the plasma would show diverse responding behaviors. which isTo examine with all the influence of the 915 MHz microwave, a 2450 MHz solid-state located between 2450 MHz and 915 MHz. Then, in the event the input microwave from Port two is 2450 orusedMHz, theof the 915 MHzshow diverse responding behaviors. filter for supply was 915 rather plasma would solid-state supply plus the low-pass To examine using the influence with the 915 MHz microwave, a 2450 MHz solid-state comparative experiments. In the experiment, 915 and 2450 MHz microwaves were insource was applied alternatively of the 915the plasma qualities and the low-pass filter for three putted from Port 2 to investigate MHz solid-state source alterations, respectively. Figure comparative experiments. Within the experiment, 915 and 2450 MHz microwaves have been inputted from Port two to investigate the plasma qualities adjustments, respectively. Figure 3 shows the impact of microwave inputted from Port two on the electron density and electron temperature measured by the Langmuir probe.Appl. Sci. 2021, 11,five ofAppl. Sci. 2021, 11, x FOR PEER Review Appl. Sci. 2021, 11, x FOR PEER REVIEW5 of eight five ofshows the impact of microwave inputted from Port two on the electron density and electron temperature measured by the Langmuir probe.Figure three. Impact of the microwave inputted from port 2 measured by the Langmuir probe: (a) electron temperature; (b) electron density. Figure three. Impact from the microwave inputted from port 2 2 measured by the Langmuir probe: (a) electron temperature; Figure three. Impact with the microwave inputted from port measured by the Langmuir probe: (a) electron temperature; (b) electron density. (b) electron density.Figure 3a shows that, when the second microwave was inputted from Port two, the plasma electron temperature ML-SA1 web progressively elevated as thewas inputted from Portpower 915 MHz microwave Figure 3a shows that, when the second microwave was inputted from Port two, the Figure 3a shows that, when the second microwave two, the incre.