In this paper we determine for the first time the volume conductivity of polyethylene (of 40 μm and 50 μm thickness), using the positive corona triode. A general theory of flowing of the current through the sample, when it depends linearly on the grid potential, is formulated. A concrete methodology for the definition of volume conductivity is composed. The volume conductivity of polyethylene lies within the interval: . These results obtained using the corona triode are closely similar to those obtained using the standardized “static” methods, thus showing its superiority to the “dynamic” method of electronic radiation.
The electrical properties of polymers are of great importance for various applications. Polyethylene is the most extensively used thermoplastic polymer, due to its excellent electrical, thermal, and mechanical properties.
Conductivity, an important parameter of polymer characteristics, is traditionally performed with the classic “static” method (a system of electrodes) [
In this paper we determine for the first time the volume conductivity of polyethylene using the positive corona triode: corona point, grid, grounded electrode.
For this purpose, firstly, a general theory of flowing of the current through the sample, when it depends linearly on the grid potential, is formulated. And then, after receiving the experimental data, a concrete methodology for the definition of volume conductivity is composed.
The results obtained by the proposed formula, are closely similar to those obtained using standardized “static” methods, thus showing a superiority of the corona triode method as compared to the “dynamic” method of electron-beam irradiation.
The current through the polymer samples is realized by the corona discharge in the point to plane geometry, described in detail in [
While a high positive voltage is applied on the corona electrode the air becomes ionized, creating positive ions and free electrons near the corona, in plasma region (
The positive ions that arrive at the surface of the sample, transfer their charge to it, introducing potential gradients on the surface and in the bulk of the sample. Thus, a part of the charges are transported along the surface and the other part are transported through the bulk, producing an electric field in the bulk of the sample [
The time variation of the first part of charges determines a displacement current and the time variation of the other part of charges determines a conduction current that depends on the kind of process that occurs in the material [
I ( t ) = S [ γ E 0 ( t ) ε + ε 0 d d t E 0 ( t ) ] (1)
where, γ , S , and ε , are volume conductivity, the surface and dielectric constant of the square sample with a length side a , respectively. E 0 ( t ) is the average electric field strength, caused by the potential difference between the surface of the sample with thickness h and the grounded electrode [
To simplify the analysis, it was assumed that surface trap states are uniformly distributed, in a thin layer [
Thus, we can write:
E 0 = V ( 0 , t ) / h (2)
Taking into consideration the Equation (2) as well as fact that S = a 2 , the Equation (1) will be presented as:
d d t V ( 0 , t ) + γ ε 0 ε V ( 0 , t ) = h ε 0 a 2 I ( t ) (3)
The volume conductivity, γ in the differential Equation (3) is the unknown quantity that we intend to determine. Meanwhile, the other quantities ( ε 0 , ε , h , a ) are known, or are experimentally determined [ I ( t ) and V ( 0 , t ) ]. But, to solve that equation, the relationship between the interdependent quantities I ( t ) and V ( 0 , t ) , should be known in advance. This raise the question: what is the relationship between I ( t ) and V ( 0 , t ) , two quantities that can be measured?
The charge density is closely related to the current across the sample and the surface potential measured. Thus, the charge condition inside the material can be represented according to the surface potential measured [
The used schematic diagram of corona triode is shown in
PE square samples of 2.5 cm side length of 40 μm and 50 μm thickness were used in this work. One face of the samples was coated by an aluminum foil, using a copper double-sided sticky layer. This ensures a good contact with the grounded electrode (circular of 20 mm diameter and 8 mm high) on which the samples were laid.
The other free surface has been exposed for 30 s to a corona discharge generated by a corona electrode (point, 1 mm diameter) situated above the grounded electrode and connected to a DC high-voltage supply (FUG HCN 14-12500). Positive 10.09 kV voltage was applied to the corona electrode. A metallic grid connected at different DC potential (Model 240 A, Keithley Instruments) of the same polarity as that of the corona electrode was inserted between the point and the sample surface. Thus, a better control over the potential to which the surface was charged, and over the charge uniformity could be achieved [
The experiments with corona triode, give us the opportunity to study the corona discharge influence in electrostatic charging process of PE. The determination of the charging current vs. grid potential curves show important results related to electrical characteristics [
We found out the relationship between the current flowing through the sample and its surface potential, via the grid potential. Therefore, two dependencies were determined simultaneously, the current flowing through the sample and its surface potential, as a function of the grid potential. The experimental graphs of both of the above dependencies, of PE (40 μm and 50 μm thickness), are shown in
The experimental results, shown in
I ( t ) = C V g (4)
meanwhile, those shown in
V ( 0 , t ) = k V g + V 0 (5)
Thus, considering the Equation (4) and the Equation (5), the required relationship between the current flowing through the sample I ( t ) and its surface potential V ( 0 , t ) is obtained and is of the type:
I ( t ) = C 1 [ V ( 0 , t ) − V 0 ] (6)
where:
C 1 = C / k (7)
Let us turn to the determination of volume conductivity γ , that is the fundamental objective of this study. The definition of the relationship between the sample current I ( t ) and the surface potential V ( 0 , t ) in Equation (6), allows us to write the Equation (3) in the following form:
d V ( 0 , t ) d t + ( C 2 − C 3 ) V ( 0 , t ) + C 3 V 0 = 0 (8)
where,
C 2 = γ ε 0 ε and C 3 = h C 1 ε 0 a 2 (9)
The solution of the Equation (8) is associated with logarithmic and exponential expressions. If the below conditions for the presentation of the logarithmic and series expansion of exponential functions:
C 3 − 1 t < C 2 < ( n − 1 n ) C 3 and C 3 < n t (10)
are satisfied, then the solution has the form:
V ( 0 , t ) = V 0 [ C 2 t + ( C 3 + C 2 C 3 − C 2 ) ] (11)
where t is the time interval in which the current flows through the sample, whereas n = V ( 0 , t ) / V 0 > 1 [
In the Equation (11), C 2 is the only unknown quantity that contains γ , the object of our determination. Related with C 2 , Equation (11) represents an equation of the second degree. The only solution that can be accepted, under our experimental conditions, is:
C 2 = C 3 [ V ( 0 , t ) − V 0 ] [ V ( 0 , t ) + V 0 ] + C 3 V 0 t (12)
as it satisfies the condition given by the Equation (10) [
γ = ε 0 ε C 3 [ V ( 0 , t ) − V 0 ] [ V ( 0 , t ) + V 0 ] + C 3 V 0 t (13)
Let us note:
C 0 = h / ε 0 a 2 (14)
that is a constant for a given sample, as h and a are the thickness and the length side of square sample, respectively.
Thus, using the constants C 0 , C , k [see Equation (7)] and the quantity n , the Equation (13) can be written:
γ = ε 0 ε C 0 C ( n − 1 ) k [ ( n + 1 ) + C 3 t ] (15)
Firstly, let us discuss about the important experimental constant k. in view of Equation (7), Equation (9) and Equation (17), the constant C 3 can be written:
C 3 = C 0 C / k (16)
Thus, according to Equation (10), we can write:
k > k 0 / n (17)
where,
k 0 = C C 0 t (18)
But, to permit the constant k tobeused in all the allowed zone of experimental measurements, itneedstobedetermined in the case when n = V ( 0 , t ) V 0 = k V g V 0 + 1 has the lowest value.
The experiments show that V ( 0 , t ) < V g , thus we may obtain:
n > n min = 1 1 − k (19)
In view of Equation (17) and Equation (19) we can conclude:
k > k 0 1 + k 0 (20)
Secondly, let us just clarify what is the conductivity zone, determined by the Equation (15).
Let us express γ from Equation (15), in its final form, as a function of k 0 and k . We have:
γ = ε 0 ε k 0 ( n − 1 ) t [ k 0 + k ( n + 1 ) ] (21)
Whereas, according to Equation (9) and Equation (10): ε 0 ε ( C 3 − 1 t ) < γ < ε 0 ε ( n − 1 n ) C 3 or using the constants k 0 and k , we obtain:
ε 0 ε k t ( k 0 − k ) < γ < ε 0 ε k 0 k t ( n − 1 n ) (22)
The above relation gives them a the matical interval of γ , valid for n > 1 . But, from the theory formulated by us, in view of Equation (5) and Equation (19), derives 1 1 − k < n < k ( V g ) max V 0 + 1 or, if we note k 1 = V 0 / ( V g ) max we have:
1 1 − k < n < k + k 1 k 1 (23)
Thereof derives that, in our argumentations, only the surface potential values that satisfy the condition:
V 0 1 − k < V ( 0 , t ) < ( k + k 1 ) V 0 k 1 (24)
are accepted. Thus, according to Equation (21) and Equation (23) as well, the interval that should be conditioned by extremum values of n , is determined as below:
ε 0 ε k 0 k t ( 1 k + α ) < γ < ε 0 ε k 0 k t ( 1 k 2 + β ) (25)
where:
α = ( k 0 + k ) ( 1 − k ) and β = k 1 ( k 0 + 2 k ) (26)
Definitely, in the theory developed by us, only those experimental facts which are subject to Equation (20), Equation (23) and Equation (24) are accepted. While γ is defined by the Equation (21) and lies in the interval determined by Equation (25).
Let us present, in the
It can be seen that the experimental constants in both cases, satisfy the condition given by Equation (20). While the acceptable coefficients, in accordance with the Equation (23), satisfy the conditions: 14.3 < n < 1080 and 14.3 < n < 1020 , respectively. Thereof derives that, [see Equation (24)], the surface potential values higher than 1020 V cannot be accepted. So, in accordance also with Equation
PE Thickness | Experimental Constants | ||||||
---|---|---|---|---|---|---|---|
C 0 ( 10 9 Ω ⋅ s − 1 ) | C ( 10 − 13 Ω − 1 ) | k ( 10 − 1 ) | k 0 ( 10 − 2 ) | k 1 ( 10 − 4 ) | α ( 10 − 2 ) | β ( 10 − 3 ) | |
40 μm | 7.23 | 1.76 | 9.3 | 3.82 | 8.64 | 6.78 | 1.64 |
50 μm | 9.04 | 1.50 | 9.3 | 4.07 | 9.09 | 6.79 | 1.73 |
(25), volume conductivities, γ in both samples, lie within the intervals: 2.36 × 10 − 14 Sm − 1 < γ < 2.72 × 10 − 14 Sm − 1 and 2.52 × 10 − 14 Sm − 1 < γ < 2.90 × 10 − 14 Sm − 1 , respectively.
A review of the literature, regarding the electrical properties of PE [
Let us compare the above results, obtained with the corona triode, with those obtained before, using standardized “static” methods (a system of electrodes) and “dynamic” methods (electronic irradiation of PE) [
The studies show [
While, using the “dynamic” methods [
It can be clearly seen that the corona triode method is superior to the “dynamic” method because its results are closely similar to those obtained using the standardized “static” methods. We emphasize that the differences, generally, are not related with the order of magnitude but only with its coefficient. As there are differences between the above mentioned methods, these differences in results are to be expected. In the first case, the positive ions of corona triode are used. In the second case, electron “bombardment” from a scanning electron microscope is used, thus the volume resistivity is dependent on electrons energy and on the irradiation time as well. While in the third case, a three electrode differently standardized system is used [
In this paper we determine for the first time the volume conductivity of polyethylene, using the positive corona triode: corona point, grid and grounded electrode. The formulated theory and the proposed methodology, when the current flowing through the sample is proportional to its surface potential, allows the precise determination of the γ interval.
The volume conductivity ( γ ) interval for PE is defined as the overlap of the two γ intervals for PE of 40 μm and 50 μm thickness.
The obtained results, using the corona triode are closely similar to those obtained using the standardized “static” methods, thus showing its superiority to the “dynamic” method of electronic radiation.
Dhima, P. and Vila, F. (2017) Determination of Volume Conductivity of Polyethylene Using Positive Corona, When the Current through the Sample Depends Linearly on Grid Potential. Journal of Materials Science and Chemical Engineering, 5, 40-51. https://doi.org/10.4236/msce.2017.512004