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METHODS OF IMPACT EXPERIMENT WITH AL2O3 AND Fe MICROPARTICLES
Ye Yicong1, Wang Libo1, S.A. Bednyakov2, S.V. Zaytsev2, L.S. Novikov
2

1 Tsinghua University, Peking, 100084 China, E-mail: yeyc@mails.thu.edu.cn 2 Skobeltsyn Institute of Nuclear Physics, Moscow State University, Moscow, 119992 Russia, E-mail: novikov@sinp.msu.ru Al2O3 microparticles and Fe microparticles are investigated under optical microscope, and their behaviors in the acceleration experiment are also examined. It is concluded that, although Fe is better charged with higher q than Al2O3, however, Al2O3 achieves a higher speed because it is lighter and hollow.

1 Introduction Al2O3 is chosen as the material used in acceleration and impact experiments for the good character ­ hollow sphere with diameter 1В2µm and wall thickness h=150В300nm, which makes it very suitable for high-speed impact experiment, because special substance can be filled into the inner part of the sphere and various phenomenon can be achieved. Besides, the tensile strength of Al2O3 is high up to ~109Pa. In this paper, the basic form of Al2O3 microparticles and their behaviors in the acceleration experiment are examined, comparing with Fe particles. 2 Experimental methods The forms of the particles were determined under optical microscope named AXIO Imager.A1m, produced by Carl Zeiss Company. The particles were accelerated in microparticle injector of MSU and their velocities and charges were measured with an A/D system, which are shown in Figure 1.

(a) Microparticle (b) System of measuring the velocity and injector charge of particle Figure 1 Equipment used in the acceleration experiments

3 Results and analysis 3.1 Particle size The forms of Al2O3 and Fe particles were examined under optical microscope (see Figure 2), and their diameter distributions were investigated using the software supplied with the microscope (see Figure 3). Although Al2O3 is much bigger than Fe, but it is much lighter (see Table 1). This is because not only Al2O3 has a lower density, but also it is hollow, while Fe particle is solid sphere.


(a) Al2O3 particles

(b) Fe particles

Figure 2 The forms of Al2O3 and Fe particles under optical microscope

(a) Al2O3 (b) Fe Figure 3 Size distribution of Al2O3 and Fe particles

3 3 o d

Table 1 Size and mass contrast between Al2O3 particles and Fe particles Particles Al2O3 Fe Sample number 204 204 230 Wall thickness h (nm) 300 150 -6 Average diameter (10 m) 1.69 1.18 -14 Average mass (10 kg) 0.747 0.444 1.07 .2 Results of acceleration experiments .2.1 Determination of the number of detectors The parameters of the separate accelerated particles were measured with the help f the two detectors K1 and K2 shown in Figure 1. The particle charge was etermined using the amplitude of pulses induced on detectors (Figure 4).
A

t

1

t

2

Figure 4 Oscillograms of signals from two ring gauges K1 (upper) and K2 (lower).

The particle velocity was determined using time of the particle flight either just in K1 (t1) or between K1 and K2 (t1+t2). The results are compared in Table 2, and it is


obvious that there are no big difference between using both of the two detectors and using only one detector. It is determined that only one detector is enough for measuring the velocities and charges of particles for the rest work. (It is true if velocities are not too large.) Table 2 Contrast between two detectors an It e m 2 detectors Sample number 64 Average speed [km/s] 0.3145863 Standard deviation 0.1254 Standard deviation of 0.0157 average Believe probability 90% Confidence 0.0256 Result 0.3146±0.0256 d one detector 1 detector 64 0.3184315 0.1410 0.0176 90% 0.0289 0.3184±0.0289

3.2.2 Velocity distribution The behaviors of Al2O3 and Fe particles in the acceleration experiments were investigated.

(a) U=10.8kV Al2O3

(b) U=18.2kV Al2O3

(c) U=20.6kV Al2O3

(a) U=13.2kV Fe (b) U=16.6kV Fe (c) U=20.6kV Fe Figure 5 Velocity distributions of Al2O3 particles and Fe particles under different voltages

Information for calculating the velocity of particles was achieved by oscillograph. Through statistical calculation, the velocity distributions of Al2O3 and Fe under different voltages are shown in Figure 5 and Table 3. It is obvious that, with the acceleration voltage increasing, the average speed of Al2O3 is increased, and under the close voltage, Al2O3 particle has a higher average speed than Fe particle. Also,


we can use higher voltage with Al2O3 than Fe without discharges in vaccum chamber.

Table 3 Comparison of average different Particles Acceleration voltage 10.8 [kV] Sample number 56 Average speed [km/s] 0.245 3.2.3 Charge distribution

velocity of Al2O3 with Fe under voltages Al2O3 Fe 18.2 20.6 13.2 16.6 20.6 64 0.315 59 0.361 63 57 59 0.20 0.22 0.28 2 4 5

With the oscillograph data of Al2O3 and Fe particles, the charge distribution can be calculated, using formula q = kA, where A is the output voltage (see Figure 4 ) and k is the known (we used calibration of amplifier) coefficient as 1.9*10-13[C/V]. The results are shown both in Figure 6 and Table 3.

(a) U=10.8kV Al2O3

(b) U=18.2kV Al2O3

(c) U=20.6kV Al2O3

U=13.2kV Fe U=16.6kV Fe U=20.6kV Fe Figure 6 Charge distributions of Al2O3 and Fe particles under different voltages

We can see that Fe particles have higher charges than Al2O3. Possible reason ­ that Fe particle is metallic, which is better for charging than non-metallic Al2O3.


Table 4 Comparison of charge distribution of Al2O3 with Fe under different voltages Particles Al2O3 Fe Acceleration voltage [kV] 10.8 18.2 20.6 13.2 16.6 20.6 Sample number 56 64 59 63 57 59 -14 Average charge [10 C] 2.02 3.57 2.64 3.99 3.82 4.01 3.2.4 Specific charge of the particles The specific charge of the particles q/m can be achieved using this formula: qU=mv2/2, and the results are shown in Figure 7 and Table 5.

(a) U=10.8kV Al2O3

(b) U=18.2kV Al2O3

(c) U=20.6kV Al2O3

(d) U=13.2kV Fe (e) U=16.6kV Fe (f) U=20.6kV Fe Figure 7 The value of q/m of Al2O3 and Fe particles under different voltages

Table 5 Comparison of q/m value of Al2O3 with Fe under different voltages Particles Al2O3 Fe Acceleration voltage 10.8 18.2 20.6 13.2 16.6 20.6 [kV] Sample number 56 64 59 63 57 59 q / m [ C/ k g ] 3.79 3.14 4.07 2.14 2.40 2.68 3.5 Analysis The results achieved in the experiments, together with theoretical calculations, are summarized in Table 6 and Figure 8, in which the obtained relation of the particle parameters with the voltage on the needle is shown. The theoretical maximum speeds of particles were calculated using formula [2]:
v
max

= (12 0 E

max

Ud -1 -1 )1 / 2 = 1.031 10 -5 ( E

max

Ud -1 -1 )1 / 2 = 0.326(Ud -1 -1 )1 / 2 [ m/s ] ,


Where 0 ­ electric constant; d, ­ diameter and density of particles, repectively; Emax ­ maximum tension of electric field with a value of 109 V/m in our condition, U ­ potential on the accelaration electrode. The theoretical maximum charges of particles were calculated using formula[3]: qmax = 0 d 2 Emax = 2.780 10-11 Emax d 2 = 0.0278d 2 [C] , Where d ­ diameter of particle, Emax ­ maximum tension of electric field, 109 V/m. The specific charge of particle was calculated using formula: q / m = v 2 / 2U , Where v ­ velocity of particles, U - potential on the accelaration electrode. It is visible that, Fe particles have experimental charge values closer to theoretical maximum than Al2O3. Although Fe is better charged with higher q than Al2O3, however, Al2O3 achieves a higher q/m and a higher speed because it is lighter and hollow. Table 6 Behaviors of Al2O3 and Fe particles under different acceleration voltage Al2O3 Fe Acceleration voltage [kV] 10.8 18.2 20.6 13.2 16.6 20.6 Experimental average speed 0.24 0.31 0.36 0.20 0.22 0.28 vexp [km/s] 5 5 0 2 4 5 Theoretical maximum speed 0.44 0.58 0.61 0.40 0.45 0.51 vmax [km/s] 9 2 9 8 8 0 0.57 0.54 0.58 0.49 0.48 0.55 vexp/vmax 7 1 2 5 9 9 Experimental average 2.02 3.57 2.64 3.99 3.82 4.01 -14 charge [10 C] Theoretical maximum 8.60 4.52 -14 charge [10 C] Experimental average mass 2.26 2.18 6.80 7.82 10.7 8.28 [10-14kg] Specific charge of the 3.79 3.14 4.07 2.14 2.40 2.68 particles q/m [C/kg]
0.36 0.32 v, km s 0.28 0.24 0.20 10 12 14 16 U, kV 18 20 22
q, 10 C
-1
-14

Al2O3 Fe

8 Al2O 6 4 2 0 10 Fe
3

12

14

16 U, kV

18

20

22

Figure 8 Particle parameters as function of the voltage on the needle

4 Conclusions As known, metal particles are more easily charged than non-metals. In this work, Fe is better charged with higher q than Al2O3, which is non-metal. However, the


hollow character of Al2O3 makes it much lighter than Fe, although Fe particle is smaller. As a result, Al2O3 has a higher specific charge q/m than Fe, and accordingly, the velocities achieved on Al2O3 particles are higher. But it is still not good enough. The size of Al2O3 is too large to achieve higher velocity.
1. Novikov L.S. High-speed impact in cosmos, Moscow, Russia, 2003 (in Russian) 2. Novikov L.S., Voronov K.E., Semkin N.D. et al. Measurement of solid microparticle flux in geosynchronous orbit. In: ESA Symp. Proc. on Environment Modelling for Space-based Applications, ESTEC, Noordwiji, NL, 18-20 September 1996 (SP-392), pp. 343-348 3. Novikov L.S., Bednyakov S.A., Soloviev G.G., Ermolaev I.K., Pilyugin N.N. Laboratory modeling of space particles impact on materials and structures. In: Proc. of the 4th Europ. Conf. on Space Debris, Darmstadt, Germany, 18-20 April 2005 (ESA SP-587), pp. 697-700