CC BY
48
DOUBLE ELECTRICAL LAYER IN THE CATHODE SPOT
Leonid I. Gretchikhina, Svetlana D. Latushkinab, Viktoryia M. Kamarouskayac
a Belarusian State Academy of Communications, Minsk, Republic of Belarus, e-mail: [email protected], ORCID iD: ©http://orcid.org/0000-0002-5385-9037 b Physical Technical Institute, National Academy of Sciences, Minsk, Republic of Belarus, e-mail: [email protected],
ORCID iD: ©orcid.org/0000-0001-5390-0991 b Belarusian National Technical University, Minsk, Republic of Belarus, e- mail: [email protected] ORCID iD: ©http://orcid.org/0000-0001-8925-6421
DOI: 10.5937/vojtehg64-9851
FIELD: Materials Science at the Nanolevel ARTICLE TYPE: Original Scientific Paper ARTICLE LANGUAGE: English
Abstract:
The paper describes a new phenomenon of the generation of the double electrical layer above the cathode spot surface. The neutralization of this layer leads to the reverse current of free electrons, generated due to negative ions ionization. The negatively charged flame of the cathode spot periodically ignites and attenuates, so the duration of the cathode spot existence is defined by this oscillating process. The reverse motion of the cathode spot in the longitudinal magnetic field takes place owing to the generation of the reverse high-power neutralization current of the double electrical layer by the electrons appearing during the negative ions ionization in the cathode flame.
Key words: electric discharge, cathode spot, cathode flame, negative ions, double electrical layer.
Introduction
The vacuum plasma coatings technique is widely used for constructional materials hardening and friction force decreasing (Baldaev, Borisov, Vachalkin, 2007), (Mrochek, Vershina, Ivashchenko, et al, 2004), (Grigoryants, 1989). The ion plasma technique is mainly applied for the
vacuum plasma coatings deposition. In this case, the vacuum arc burns in the plasma material of the cold cathode due to its discharge current sputtering. This technique is quite complicated to be applied as it is difficult to determine the processes taking place inside the cathode spot and which plasma composition can occur in the cathode flames of the arc discharge.
The processes occurring inside the cathode spot were studied in detail by (Kesaev, 1968). As a result, the fundamental characteristics of the cathode spots were determined as well as the main directions of further investigations. The spectroscopic investigations of the cathode spots and the explosive processes occurring in the cathode flames were specially investigated by Kesaev. He investigated in detail the effect found by Shtark in 1903, where the cathode flames in the tangential magnetic field are not deflected in accordance with Ampere's law (even nowadays this effect has no convincing explanation).
The problems raised by Kesaev are solved to a certain extent, but not completely. The spectroscopic investigations of the cathode flames of the arc and sparkle discharges were carried out by Gretchikhin together with colleagues in the middle of the 1960s and it is shown that the plasma generation in the cathode flames is determined by the presence of negative ions inside the flames (Gretchikhin, Tyunina, 1967), (Gretchikhin, Davydov, Minko, Ya, 1968 ), (Gretchikhin, 1974).
The explosive processes investigations in the cathode flames were carried out by Mesyats with colleagues and it was found that micro explosions can be generated inside the cathode spots on separated low-sized particles, called ectons, (Mesyats, 2000), (Mesyats, 1993), (Mesyats, 1995).
During the vacuum plasma technique development, some new problems appeared, such as: 1 - why there is the presence of the liquid phase under micro explosions in the cathode spot; 2 - what processes determine the electron energy distribution, and, consequently, why the percentage ratio of the ions with a different degree of ionization does not correspond to Saha equation; 3 - why the cathode flames under the longitudinal magnetic field application do not deflect in accordance with Ampere's law, etc. In this regard, there is a goal to develop the model of erosion plasma generation which could quite convincingly describe the character of the plasma generation in the high-current vacuum arc. So, the following actions should be taken to solve the given tasks:
- to develop the exact model of the micro explosion in the cathode spot with regard to negative ions generation;
- to study the effect considering the cathode spot heating and liquid phase generating;
- to find out the processes leading to the electronic component plasma heating and to prove the percentage ions composition in the cathode flame in accordance with experimental data; and
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- to find the cause of the reverse motion of the cathode flame in the longitudinal magnetic field.
Therefore, we consistently considered all the raised issues as applied to the erosion plasma of the cathode spots.
Negative ions in the explosive processes
Only the external atoms of the separate cathode material cluster are in contact with surrounding atoms during an explosion in the cathode spot. Cluster ionization energy is lower than 2 eV (Gretchikhin, 2008), while the energy of the electron affinity of an atom is slightly lower (Messi, 1979). Under the melting point, due to the tunnel-effect, the valence electrons of the surrounding atoms and clusters transverse to the atoms of the explosive cluster. The cluster is split onto separate free atoms in the moment of explosion. The built-in dipole electrical moments of the free atoms in the electric field of the cathode potential drop are lined in the field so the positive charge is in contact with the cathode material surface. The energetic scheme of the cluster atom interaction with the cathode surface is shown in Fig.1. The probability of this is determined by the transparency ratio of the potential barrier during the tunnel-effect:
n
W = = exp n
(i)
where d = ra - rk -difference between the atom radius and its covalent radius; E1 - cluster energy ionization of the cathode material; E2 - energy of the electron affinity of an atom; me - electron mass.
As an example, the following cathode materials can be examined: iron, titanium, and copper1.
Not all of the cluster atoms of the surface layer are directly in contact with atoms and clusters of the surroundings. Taking this into consideration, the general probability of the fact that titanium atoms leave the cathode spot by means of negative ions is:
N, -AN,
W =_cL_cL w (2)
gen. N
cl.
Here Ncl. - general number of particles in the cluster and LNct -number of particles of the surface layer which are not in direct contact with surrounding atoms of the cathode material.
1 The choice of these materials is explained by the difference in the crystal structure.
Figure 1 - Scheme of the negative ions generation in the cluster explosion process: a) - model of the cluster atoms interaction with the substrate and b) - model of the electrical charge separation during vapor ejection after a cluster explosion Рис. 1 - Схема образования отрицательных ионов в процессе взрыва кластера: а) - модель взаимодействия атомов кластера с основой и б) - модель разделения электрических зарядов при выбросе пара после взрыва кластера Slika 1 - Sema obrazovanja negativnih jona tokom procesa eksplozije klastera a) - model interakcije atoma klastera sa substratom i b) - model separacije naelektrisanja tokom izbacivanja pare nakon eksplozije klastera
For example, iron clusters have the bcc structure, where there are 9 diatomic molecules, out of which only 4 molecules are in contact with the cathode material. The cluster radius is rci. = 3.78 A, the cluster ionization potential - E1 = 1.46 eV (Gretchikhin, 2008), the negative ion potential -E2 = 0.163 eV, and the difference between the atom radius and the
covalent radius is - d
'■Га - rk
■ 0.455 A. On the basis of these data, the
concentration of negative iron ions in the cathode flame of the vacuum arc is Wgen. ~ 0.261
Titanium clusters have the fcc close-packed structure, where only 9 from 13 triatomic molecules are directly in contact with the surroundings. So only these 9 molecules are negative ions, and the cluster radius is rcL = 4.38 A, the cluster ionization potential - E1 = 1.53 eV, th e negative ion potential - E2 = 0.079 eV and Wgen« 0.115.
Copper clusters have the fcc structure, where there are 13 triatomic molecules, out of which only 8 molecules are in contact with particles from the surroundings. The cluster radius is rcL = 3.84 A, the cluster ionization potential - E1 = 1.633 eV (Gretchikhin, 2008), the negative ion potential - E2 = 1.228 eV, and the difference between the atom radius and the covalent radius - d = ra -rk = 0.482 A. On the basis of these
data, the concentration of negative copper ions in the cathode flame of the vacuum arc is Wgen.~ 0.150
The passage of discharge current of the cluster length, i.e. its diameter is:
t = 2rcl / v = 2 ■ rd-Je~r / c, sec. (3)
Here rcL - the minimum radius with a separate emissive cell in the cathode spot i.e. the cluster radius, c - speed of light in vacuum, and er -relative dielectric medium permeability.
The electric polarization theory for metals was developed by (Gretchikhin, Physics, 2008) and the calculations were made for the relative permeability for natrium, aluminum, iron and copper, while the relative dielectric permeability for titanium was calculated separately and was £r~ 3.965-1013. On the basis of (3), the passing time of the electromagnetic wave through the cluster is t - 1.085 10-11 sec for iron, t= 1.8410-11 sec for titanium and t= 5.5110-11 sec for copper.
This time is necessary for the cluster to absorb discharged current energy. Since the process time is ~ (1 ■ 5 )10-11 sec, the cluster destruction process has an explosive behavior. The pressure, emerging at the cluster explosion moment, can be calculated by the formula:
N
Pmax. = 73 kBTboil. . (4)
(2 ■ rcl.)
Here Nci - number of cluster particles multiplied by the number of atoms in the particle. Considering the overall atoms number in the cluster, the pressure at the cluster explosion inside the cathode spot is 1.82 109 Pa for iron, 1.98 109 Pa for titanium and 3.35 109 Pa for copper. Such pressure values can occur during the explosive blast (Gretchikhin, Rubleva, 2006), (Litvinskiy, 2006).
During the cluster explosion, a number of negatively charged particles are emitted from the cathode spot2. In this case, the electric current density of the charge separation during the flame discharge in the cluster explosion with double electrical layer generation is:
N W e
cl gen
Jk =—v-v/, (5)
cl
where VcL - the cluster volume and vf - the flame emission rate from the cathode spot and it is determined by using the point explosion model.
2 The attention was paid to this effect in the late 19th and at the beginning of 20th century (Kesaev, 1968).
The shock wave rate in solids for the point explosion is determined by the formula (Korobeinikov V. P., Melnikova N.S., Ryazanov E.V. 1961) and (Kostenboim X.S. 1974)
v h = —
sh.w. 5
Y E ^
1/2
api
1 (6)
C
r 3/2 'cl.
where a ~ 0.851, E0 - energy emitted in the cluster during the current discharge flow and pc - the cathode material density.
The energy emitted in the cluster is:
nd2
W = Lmax t , J (7)
where Lmax - the Poynting vector, dK - the cathode spot size and t - the electromagnetic wave passage time through the cathode material cluster.
On the basis of the cathode spot "autographs", it is shown in this work (Kesaev I.G. 1968) that the cathode spot diameter is increased due to arc current and film thickness. When the arc current and films thickness are quite small, the ratio of the discharge current to the "autograph" width is sufficiently small, and it is stabilized with a current and film thickness increase. When the arc current and films thickness are high, the ratio of the discharge current to the "autograph" width increases quickly. In the first case, not all the discharge current power is used for the film evaporation, while under the high currents and film thicknesses the spot size significantly enlargers due to "autographs" edges melting. Taking this into consideration, the probable "autograph" size of the separate copper cathode spot is (1 ■ 2) -10-5 m (the average value for further evaluations is dk = 1.5 10-5 m3).
The cathode spot is only influenced by the arc discharge current, so the average current density is - Jk = 41 / ndj.
In this case, the Poynting vector is defined by the Joule law
Lmax = JkUk , (8)
where Uk - a near-cathodic potential drop. The average values of the near-cathodic potential drop are listed here (Kesaev, 1968) and it is quite
3 Since the magnetic pressure of the current discharge is equal to the gas-kinetic pressure in
the cathode flame, then the pressure in the cathode flame at this spot diameter ~ 9.0105 Pa.
Such a quick pressure drop in the cathode flame while exiting the cathode spot is caused by
the discharge-like "vacuum expansion".
convincingly shown that this potential drop coincides with first atoms ionization potential of the cathode materials for most metals.
As a result, the flame discharge rate of the cathode flame can be calculated by means of the point explosion model and it is 4324 m/s for iron, 4652 m/s for titanium and 7820 m/s for the copper cathode. During cathode processes modeling of the pulsed discharge by laser, the flame discharge rate at some distance from the surface turned out to be 3900 m/s (Gretchikhin, Minko, 1967), while in the vacuum arc - 12.5 km/s under an arc current of 115 A (Kesaev, 1968). The flame discharge rate was 8.8 km/s for the iron cathode under an arc current of 142 A (Kesaev, 1968), while these investigations were not carried out for the titanium cathode. 1968). The found values are quite reliable and they can be used in further calculations. Then the current density, caused by the negative ions discharge from the cathode spots is ~ 4.61012 A/m2 for the titanium cathode spot, ~ 1.371013 A/m2 for iron and ~ 1.31013 A/m2 for copper. Exactly the same current densities were experimentally found during the ecton explosion (cluster) (Mesyats, 2000), (Mesyats, 1993) and (Mesyats, 1995).
The energy to be transferred to the cluster to disintegrate it into separate atoms is:
m
AQ = — AH bo»,, (9)
—
where mcl - the cluster mass, — - the cathode material molar mass AHboil -the sublimation heat. This energy is 1.75 eV for the iron cluster, 3.46 eV for the titanium one and 1.92 eV for the copper one. Using these values of energy, it is possible to determine the maximum current density which leads to the complete cluster disintegration into separate atoms by the formula:
j . (10)
J max. t t c v '
UkSkTk
Here Uk, Sk and Tk - the cathode potential drop, the cluster area and
the passage time of the cluster length by the discharge current, respectively. The near-cathodic potential drops are listed here (Kesaev, 1968) and (Kolesnik, Kolesnik, 2009), while the cluster radius values are given in (Gretchikhin, 2008). The passage time is determined by the rate of the electromagnetic waves in the cathode material and is equal to
Tk = 2rcl -yfeT / c (er - relative dielectric permeability of the cathode material
and c - the speed of light). The limit current density leading to the complete
cluster destruction is respectively 1.4109 A/m2 for the iron cluster, 2.3-109 A/m2 for titanium and 4.7108 A/m2 for copper. Therefore, the current density emerging during the cathode cluster explosion in the vacuum arc is significantly higher than the current density of complete cluster destruction. The average current density on the cathode spot is about ~ 1012 A/m2 when the discharge current is 100 A. The clusters of almost all cathode materials explode and disintegrate into separate atoms under this current density and they are discharged as a vapor-gas phase from the cathode spot.
The electric current is generated by every cluster explosion -Ik = jkSk, and the number of clusters to be exploded simultaneously in
the cathode spot is - nk = I /Ik = I / jkSk. When the current discharge is
100 A, the total number of clusters is nk = 2.86 107 for the titanium
cathode, nk = 1.63 107 for iron and nk = 1.32107 for copper. When the
cathode spot diameter is 10-5 m, the total number of clusters is nk n =
1.3108 for the titanium cathode, nk n = 1.75 108 for iron and nk n =
1.7108 for copper. It should be no more than 5 erosion cells for the titanium cathode, no more than 10 for the iron cathode and no more than 12 for the copper cathode under a current discharge of 100 A (Kolesnik, Kolesnik, 2009). It was found that the number of erosion cells in the cathode spot was within 4-12, depending on the discharge conditions. This is confirmed by estimations on the basis of negative ions emission.
The electric current is generated by every exploded cluster, and all these currents produce the emission cell with public electric current which is equal to the current discharge to that fact. Owing to this, parallel currents are integrated by the Ampere force, and this effect is called current discharge pinching.
During the clusters explosion, the electric current is conducted by negative ions, but not free electrons. The magnitude of the pulse current during every separate cluster explosion corresponds to experimental data, found by (Mesyats, 2000), (Mesyats, 1993) and (Mesyats, 1995).
The negative ions ionization takes place during flame discharging. Free electrons can be generated and they try to neutralize the positive charge on the cathode spot surface. The reverse electric current can be generated and its value is several times higher than the main discharge current.
The enormous reverse current is caused by the free electron flow and this flow is spread all over the whole cathode spot area. Having passed the near-cathodic potential drop, these electrons penetrate into the skin depth and transform this layer into a liquid film.
Liquid phase generation in the cathode spot
During a cluster explosion, the explosive emission of the negative charge from the cathode is defined by the electric current conducted not by free electrons, but by negative ions. At the same time, the positive charge is by the negative charge flame, and the double electrical layer is formed. The negative ions disintegration in the vacuum arc electric discharges takes place owing to the following reactions:
A~ + B ^ AB + e;
(11)
A + e ^ A + 2e.
Both reactions (11) occurred in the vapor-gas phase. Based on the first reaction, the concentration of generated free electrons per unit time is equal to:
dn
= kfn-an'a = kfWgen(l -WgeJnl. (12)
Here kf - the constant of the first direct reaction (11). The activation energy of the fist reaction (11) is determined by the empiric formula (Benson S., 1962).
Ea = 0,29 D - 22,2 KJ/mole, (13)
where D - the dissociation energy of the formed diatomic molecule (AB). The dissociation energy is 1.2 eV for Ti2, and - 2.05 eV for Cu2 (Radtsig, Smirnov, 1980). So the activation energy is 11.38 kJ/mole for titanium, and 35.16 kJ/mole for copper. The constant of the direct chemical reaction (Benson S., 1962) is:
kf = 2(ra + rb )
( 2nkbT Y" f Ea 1
exp
V kbT J
(14)
v — j
here ra and rb - the covalent radii of the interacting particles,
m mb
— = —--the reduced mass and ma, mb - the interacting particles
ma + mb
masses. So the constant of the first chemical reaction (11) under the boiling temperature is 3.245-10-16 m3/sec for titanium, and 6.283-10-17 m3/sec for copper.
The mass loss from the solid surface in the presence of negatively charged particles in the flow should be considered as a charged continuum flow with a double electrical layer creation. In this case, the mean free path of every negative ion in the flow must be significantly
smaller than the distance, i.e. the negative ions to be removed without the collision in the double electrical layer. So
l << L
mav 2
2eE„
(15)
Here ma - the particle mass in the cathode flame, Ee
Nalw -Sk£0
the electric field strength of the charged cathode spot surface Sk and £0 = 8.854-10-12 F/m - dielectric vacuum permeability.
There are the electric field intensity values in the double electric layer and its layer size in Table 1.
Table 1 - Main parameters of the double electrical layer Таблица 1 - Основные параметры двойного электрического слоя Tabela 1 - Nominalni parametri dvostrukog elektricnog sloja
^\Parameters Cathode^^ material Uk, V Ee, V/m Vf, m/sec Д, m Ср, J/kgK Pe, Vm l0, mm Tp, К
iron 11.8 481 4324 2.35-10-4 975 8.6-10-8 11.2 2650
titanium 6.8 459 4652 3.5510-4 684 4.2-10-' 11.7 2270
copper 11.3 1060 7820 4.84-10-4 451/513 1.610-8 19.5 2070
The mean free path in the discharge chamber is:
l
4rk
42nw '
(16)
where PC - the cathode flame pressure and rk - the radius of particles of the cathode flame (atoms for titanium and copper). The mean free path in the cathode flame is 2.76-10"10 m for titanium atoms, 2.28-10"10 m for iron and 1.86-10"10 m for copper, while the distance, the negative ions to be removed from the cathode spot surface, is 5.5 mm, 11 mm and 12 mm for iron, titanium, and copper, respectively. The condition (15) is satisfied, so the cathode flame should be considered as a charged continuum flow. In such a flow, the negative ion range distance from the cathode spot surface is determined not only by the slowing down of the charged particles in the electric field of the double layer, but also by their ionization due to the reaction (11). Then the free electrons concentration along the axis X at the distance x in the layer dx is defined from the chemical reactions and slowing down in the double electrical layer in the following way:
dX (17)
dne = kfnani
eE„
v
x
0
maV0
The solution of the differential equation in terms of the boundary condition offers the following approximate dependence for the first and second reaction (11) to occur in the flame
m v
ne (X) = ne,0 + 2kf,1nagrad (ni X
eE„
mv
ne (X) = ne,x + 2kf,2 negrad (n- X
(18)
eE
where ne0 - the initial free electrons concentration to be determined by the boiling temperature using the Saha equation.
The first reaction (11) takes place at the beginning and the high-energy ions are generated. After their appearance, the negative ions ionization by an electron impact is stimulated with the decreasing of the quick energy of exciting and forming electrons. Thus, free electrons are generated at the distance of A/ ~ 10-2 m from the cathode spot surface in accordance with reaction (11). Free electrons under the influence of the positively charged cathode spot surface are directed to the cathode, generating a reverse electric current which is equal to:
I = en,JV,Sk. (19)
where Ve - the drift electron velocity in the cathode flame plasma.
The following equality is true under stationary conditions on the basis of the charge conservation law
n-VfSkp = neJcVeSk . (20)
On the basis of (20), the reverse electric current is equal to the electric current to be generated during a cluster explosion, i.e. to the electric charge separation current with creating a double electrical layer. The difference is that the charge separation current lasts during the clusters explosion, while the reverse current lasts during the creation of the double electrical layer. The direct current is determined by the complex exploded cluster, while the reverse current - by the whole cathode spot surface. As a result, the reverse current density is an order of magnitude lower than the charge separation current.
The complete ionization of negative ions takes place at the distance of the full ions slowing down and in fact the reverse current stops. In this moment, the cathode spot stops its functioning at the given place and the cathode spot is generated alio loco. The cathode spot duration is 2.610-6 sec without dependence on the cathode material and it turns out to be the cathode spot lifetime. If the breakdown of the near-cathodic space
takes place inside the cathode space, then the cathode spot lifetime increases. This fact was experimentally proved and the most probable value was in a great agreement with data listed here (Kesaev, 1968).
Since the reverse current is transferred by electrons, they can penetrate to the skin depth (A). The specific skin layer values for some materials are listed in Table 1. The temperature of the skin layer to be heated, is:
jkukh
ApCpvf
Tp = T0 + 0 . (21)
The results of the temperature evaluations and the skin layer to be heated in the cathode layer are listed in Table 1. The surface layer heating in the cathode spot for all the metals is not higher than the boiling temperature and is slightly higher than the melting point.
The cathode spot temperature measured experimentally by an optical pyrometer under different discharge conditions was in the range of 1300 -2300 K, and 2300 - 3700 K for the copper arc. The temperature evaluations listed in Table 1 are in good agreement with experimental data and are within the melting point and the boiling temperature.
Electronic component temperature in the cathode flame
As a result of the first reaction of (11), the electrons are in the surroundings with average energy, which is equal to the difference between the diatomic molecule dissociation energy and the affinity energy:
Ee = D -07. (22)
E = 1.2 -0.163 = 1.037 eV for iron, E = 1.2 -0.079 -1.121 eV for
e ' e
titanium and Ee = 2.05 -1.228 - 0.822 eV for copper. Such average
energy of the generated electrons is enough for titanium and copper to effectively ionize by the electron impact the remaining negative ions in accordance with the second reaction (11). These free electrons during negative ions ionization generate a cloud of free electrons with an average energy of (Gretchikhin, Kudryashov, 1970)
0e = 0,550" eV. (23)
For example, in the cathode flame, consisting of iron vapor, where the continuous negative ions disintegration due to the electron impact takes place, the average electrons energy in plasma is 0.09 eV, and it corresponds to the electron gas temperature Te,2 = 1040 K; , the average
electrons energy for the titanium vapor is 0.0435 eV, so the electron gas temperature is Te,2. ~ 505 K; while for the negative copper ions it is ~ 0.452 eV with an average-effective temperature of Te,2 ~ 5243 K. So, for the vacuum arc discharge plasma in iron and titanium vapor, the electron gas energy is primarily defined by the first reaction of (11) and the values are 0.570 and 0.616 eV, while the temperatures are ~ 6620 and 7152 K, respectively. For the arc discharge copper plasma, in the first reaction the electrons are generated into plasma with 0.452 eV, while in the second reaction, with 0.675 eV. The second reaction of (11) leads to a quick electron gas temperature drop in the titanium atmosphere, just on the contrary to the copper atmosphere. So, the electron subsystem in the vapor-gas phase of iron, titanium and copper in the cathode flame has an expressed two-humped energies distribution.
Every electron generated after the first reaction (11) excites the following number of direct negative ions by means of the second reaction of (11):
1 E ^
n ~77• IT if (E,Ti)dE. (24)
3,5 E2 3,5E2
where E1 - the average energy of the generated electrons owing to the first reaction of (11) and E2 - owing to the second reaction of (11). The factor 3.5 is determined by the maximum ionization cross-section during the electron impact. (Physical magnitudes: Handbook, 1991)
The final distribution of the generated electrons due to negative ions ionization:
f (E )dE = fET)fE^. (25)
i [(E, Ti) + f2 (E, T2)\iE
In copper vapors, the electron gas temperature corresponds mainly to the second reaction of (11). Bearing in mind that there is the electron subsystem in the thermodynamic equilibrium, the average temperature of the vacuum discharge electron component in the copper vapors is ~ 7830 K. The average electron flame temperature was calculated near the surface by modeling the energy fluxes to occur in the cathode spot of the vacuum arc by means of laser, carried out by (Gretchikhin, Minko, Ya, 1967), and it was 7900 K. This coincidence was quite convincing within measurement errors.
So the electron component temperature is defined by the negative ions ionization processes. When the flame leaves the cathode surface drop, it has the temperature which is equal to the cathode material boiling temperature. And the electron flame temperature increases when the
distance from the cathode surface increases too. This was experimentally found here (Gretchikhin, Tyunina, 1967), (Gretchikhin, Davydov, Minko, Ya, 1968), (Gretchikhin, Minko, Ya, 1968), (Gretchikhin, 1974).
The following fact was found experimentally in these studies (Gretchikhin, Tyunina, 1967), (Gretchikhin, Davydov, Minko, Ya, 1968), (Gretchikhin, Minko, Ya, 1968), (Gretchikhin, 1974). High-power continuous radiation can appear near the cathode surface, but the spectral lines and bands radiation of atoms and molecules are absent. So the flame emission near the cathode surface corresponds to the condensed media, i.e. in this case it is a liquid phase. The separation between the vapor-gas and the liquid phase takes place as the distance from the cathode surface increases. The temperature quickly increases in the vapor-gas phase and atoms and molecules radiation takes place, while the liquid phase radiation disappears due to its cooling under the dispersion.
The electrons are directed onto the cathode as the negative ions disintegration and they neutralize the induced positive charge, spread all over the cathode spot. The positive ions from the discharge gap cannot reach the cathode surface, since they are neutralized during the impact with the cathode flame. The current from the discharge onto the cathode stops and so the near-cathodic area breakdown takes place in the other place and this is determined by the fact that the opposite currents are mutually repelled.
If we assume that there is vacuum arc discharge plasma in the thermodynamic equilibrium, the ion plasma composition in the cathode flames vapor inside the discharge gap can be defined by the Saha equation:
nMne 2Z
f n
i+1 er'' i+1 „„„ i +1
n.
C '—— exp
v KT j
(26)
(2пт к T)
where C = --e 3ъ ' = 2,415-1021 T3/2 - the dimensional constant;
h3
Zi+1, Zi - the statistical partition function; £м,£, - the energy of state /+1
and i the degree of ionization of plasma particles, kb - the Boltzmann constant, Т - the corpuscular heated vapor temperature, me - the electron mass and h - the Planck constant.
Table 2 - Ions per cent of different degree of ionization Таблица 2 - Процент ионов разной кратности ионизации Tabela 2 - Procenat jona razlicitog stepena jonizacije
Element Uk, Ions fraction, %
V I II III
Ti 6.8 27/27 72/67 1/6
Cu 11.3 30/30 68/54 1.9/15
CO
o
co
"o >
CD
O CM
of
UJ
a.
Z) O
o <
o
X
o
LU
H >-
OH <
H
<
CD >o
X UJ
H O
O >
The direct measurements of the composition by percentage of ions with different degrees of ionization were carried out in the vacuum arc discharge at a current of 100 A. (Mrochek, Vershina, Ivashchenko, et al, 2004) and (Kolesnik, Kolesnik, 2009) and the results are listed in Table 2 (the lower row). If we make the association with the composition by percentage of ions with the first degree of ionization, then, in accordance with the Saha equation, the temperature is ~ 4100 K for the titanium cathode and 6830 K for the copper cathode. Under these temperatures, the composition measurements by percentage of ions with consequent degrees of ionization in the vacuum discharge are listed in Table 2 (the upper row). The found results of the composition by percentage using the Saha equation do not obviously correspond to the composition by percentage obtained by direct measurements. It indicates that the generated plasma in the vacuum arc discharges is essentially no equilibrium. There is a difference between the electronic temperature and the atomic temperature obtained by the Saha equation. The electronic component in the vacuum arc plasma discharge has the electrons with different energy, i.e. their generation takes place due to the different mechanisms on the basis of reactions in (11).
Electric current reverse motion in the cathode flame under the tangential magnetic field
It was found experimentally by Shtark and then by Keasev in detail, that the reverse current rate of the cathode spot under the longitudinal magnetic field depends on:
- cathode material;
- cathode material surface condition;
- arc current;
- oxide film;
- cathode temperature; and
- pressure of reaction discharge gas in the chamber.
The simultaneous explosions of several clusters (emission cells systems) in the cathode spot leads to the double electrical layer generation above the cathode spot of a sufficiently great size (l0 Table 1). The electrical current of neutralization of the positive charge on the cathode spot surface in the double electrical layer is directed oppositely to the principal discharge current. The Ampere force appears under the magnetic field superposition along the cathode surface:
Hence, the cathode spot rate of motion is:
Vn = = ~1- [ BJ, (28)
mk vf mkvf
where mk - the cluster mass.
Let it be examined in what way the above-mentioned changing parameters have the influence on the cathode spot velocity of reverse travel under the longitudinal magnetic field.
The material cathode dependence is directly proportional to the dependence on the squared double electrical layer width and inversely proportional to the dependence on the cluster mass and flame rate of motion for different materials. The titanium cathode spot rate of motion is 5.8 times higher than the one for iron, while for copper it is 7.2 times higher.
The dependence on the surface condition (i.e. roughness) occurs when the cathode spot fails and recovers in another area, but the transition from one hill to another with a roughness increase cannot take place and the cathode spot motion stops.
The cathode spot rate of motion increases directly proportionally to the arc current under constant other parameters.
The oxide film on the cathode material prevents the near-cathodic space breakdown and it can lead to the quick cathode spot motion stop.
The cathode temperature increase leads to the thermo emission current increasing, which reduces the reverse electron neutralization current of the double electrical layer. Therefore, it decreases the Ampere force and, consequently, the cathode flame rate of reverse motion.
The increase of the pressure of reaction discharge gas in the chamber leads to the increase of the positive ions concentration in the discharge gap. The cathode flame is bombarded by positive ions, the negative ions concentration is decreased and, consequently, free electrons concentration during the negative ions ionization is decreased, too. The reverse electric current is reduced and the cathode spot rate of reverse motion is decreased.
Conclusion
Therefore, the investigations of the vacuum arc discharge with the cold cathode allowed finding out a new phenomenon. During the generation of a defined complex clusters explosion in the cathode spot, a fraction of certain atoms is as negative ions. As a result of this, a double electrical layer is formed above the cathode spot, and its neutralization leads to reverse current of free electrons generated owing to the negative ions ionization.
This phenomenon in the cathode spots of the arc discharges allowed finding out the following:
1. The negative charged flame with frequency, defined by the cathode spot life time discharges from the cathode spot,
2. The double electrical layer is generated above the cathode spot surface, which is neutralized by the reverse electrical current, generated by free electrons owing to the negative ions ionization,
3. All the phenomena taking place during the cathode spot motion under the longitudinal magnetic field are explained by the high-power reverse neutralization current generation of the double electrical layer.
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ДВОЙНОЙ ЭЛЕКТРИЧЕСКИЙ СЛОЙ В КАТОДНОМ ПЯТНЕ
Леонид И. Гречихина, Светлана Д. Латушкина6, Виктория М. Комаровскаяв
а Белорусская государственная академия связи, г. Минск,
Республика Беларусь, 6 Физико-технический институт НАН Беларуси, г. Минск,
Республика Беларусь, в Белорусский национальный технический университет, г. Минск, Республика Беларусь
ОБЛАСТЬ: материалы, нанотехнология,
материаловедение на наноуровне ВИД СТАТЬИ: оригинальная научная статья ЯЗЫК СТАТЬИ: анлийский
Краткое содержание:
Установлено новое явление, заключающееся в образовании над поверхностью катодного пятна двойного электрического слоя, нейтрализация которого приводит к обратному току свободными электронами, образующихся вследствие ионизации отрицательных ионов. Отрицательно заряженный факел из катодного пятна периодически пропадает и возникает. Этот колебательный процесс определяет длительность существования катодного пятна. Обратное движение катодного пятна в продольном магнитном поле происходит вследствие образования обратного мощного тока нейтрализации двойного электрического слоя электронами, возникающих при ионизации отрицательных ионов в катодном факеле.
Ключевые слова: электрический разряд, катодное пятно, катодный факел, отрицательные ионы, двойной электрический слой.
РУОБТРиК! ЕЬЕКТтСМ БЬОи и КАТОРЫОМ БРОТи
Leonid I. Згес^т3, Svetlana Р. 1_аШёк1паЬ, Viktorija М. КотагоУ8ка]ас а Ве!огиБка с1гёаупа акас1етуа 2а БаоЬгаса] I Ув2е, М1пБк,
РериЬНка Ве!огиБуа Ь !пБйМ 2а ^ки I 1еИп1ске паике РгЁаупе акас1етуе паика, М1пБк,
РериЬНка Ве!огиБуа с Ве!огивк1 пас1опа1п1 1еИп1ск1 итуегейе^ М1пБк, РериЬНка Ве!огив1]]а
ОВЬАБТ: т^егуаП, папо1е1то!одуе УРБТА С1_А1\1КА: ог1д1па!п1 паисп1 с!апак ^!К С1_А1\1КА: епд!евк1
Sazetak
U radu se opisuje novootkrivena pojava stvaranja dvostrukog elektricnog sloja iznad povrsine katodnog spota. Njegova neutralizacija dovodi do reverzne struje slobodnih elektrona, generisane usled joni-zacije negativnih jona. Negativno naelektrisan plamen katodnog spota periodicno se stvara i gasi, tako da je duzina postojanja katodnog spota definisana ovim oscilirajucim procesom. Reverzno kretanje katodnog spota u longitudinalnom magnetnom polju desava se zahvaljujuci generisanju reverzne struje neutralizacije velike snage dvostrukog elektricnog sloja pomocu elektrona koji nastaju tokom jonizacije negativnih jona u plamenu katode.
Kljucne reci: elektricno praznjenje, katodni spot, plamen katode, negativni joni, dvostruki elektricni sloj.
Paper received on / Дата получения работы / Datum prijema clanka: 25. 12. 2015. Manuscript corrections submitted on / Дата получения исправленной версии работы / Datum dostavljanja ispravki rukopisa: 27. 03. 2016.
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© 2016 Авторы. Опубликовано в "Военно-технический вестник / Vojnotehnicki glasnik / Military Technical Courier" (www.vtg.mod.gov.rs, втг.мо.упр.срб). Данная статья в открытом доступе и распространяется в соответствии с лицензией "Creative Commons" (http://creativecommons.org/licenses/by/3.0/rs/).
