plasma sources & wave propagation

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Plasma Sources & Wave Propagation Presented by Dr. Mahmoud Saad Afify Department of Physics, Faculty of Science, University of Benha

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Page 1: Plasma Sources & Wave Propagation

Plasma Sources &

Wave Propagation Presented by

Dr. Mahmoud Saad Afify

Department of Physics, Faculty of Science,

University of Benha

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Outlines

• Introduction

• Cold and thermal plasma

• DC glow discharge, RF, Microwave, and

pulsed plasma

• Observations of waves in plasma

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The fourth state of matter “Plasma”

Add more energy

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Plasma sources

Cold plasmas are those with low pressure

and Te >> Th. It is obtained in DC discharge,

RF discharge, and short pulse discharges.

Thermal plasmas, are those with high

pressure and Te~Th. It is produced

in plasma arc.

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DC discharge

plasma

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DC discharge experiment

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The negative glow is mostly field-free, E ≈ 0. In the

positive column, the axial electric field is constant.

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Mean Free Path

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Radio Frequency Discharge

1. In RF plasmas, Conductive and

nonconductive electrodes can be

used.

2. RF plasmas can be sustained

with internal as well as external

electrodes.

3. RF plasmas are characterized by

higher ionization efficiencies.

4. RF plasmas can be sustained at

lower gas pressures.

5. In RF plasmas the energy of the

ions bombarding the sample is

controlled.

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Microwave Plasmas

1. The excitation of the plasma

by microwaves is similar to

the excitation with RF, while

differences result from the

ranges of frequencies.

2. Also, it is difficult to sustain

Microwave discharges at low

pressures (< 1 torr)

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Electron Cyclotron Resonance

Plasmas

1. It can sustain at low

pressures.

2. High ionization efficiency.

3. Wide range of achievable

ion energies.

4. Electrodeless coupling of

the electric power to the

plasma.

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Linear Z-pinch device

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Visualization of pinch effect

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In any electric circuit, there can be three basic

components: resistance, capacitance, and

inductance, in addition to a source of emf. (There

can also be more complex components, such as

diodes or transistors.)

Because some resistance is always present,

electrical oscillators generally need a periodic

input of power to compensate for the energy

converted to thermal energy in the resistance.

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The energy stored in the electric field of the

capacitor at any time t is

the energy is stored in the magnetic field of

the inductor. At any time t,

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Collective behavior

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Reason for Fourier series

Plasma oscillation could be propagated and so we have a wave.

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Recall that any wave has three basic properties:

1) Amplitude – the height of the wave

2) Frequency – a number of waves passing through in a given second

3) Phase – where the phase is at any given moment.

# According to Fourier, any periodic function can be represented by an

infinite series of sinusoidal functions with frequency ω and wavelength λ.

# The Exponential Fourier Series is

where we consider the periodic function to be the plasma density as an

example. Also, we consider 1D only.

By convention, the exponential notation means that the real part of the

expression is to be taken as the measurable quantity.

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The concept of Modulation

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