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Study of Dust Detection System on a Micro Satellite
Space Systems Dynamics Laboratory
M2 Kyohei Nakashima
2
Contents Objective Background Dust Detection System Acoustic Emission Method Experiments Results Conclusions
3
Objective
Analysis and verification of dust detection system on a micro satellite using Acoustic Emission sensors
4
Background
Space weather forecast is necessary because space disasters threaten human space activities. Space disasters
Magnetic storm High energy particles
radiation Space debris
Sunflares
Space debris
Radiation
Earth
Magnetic storm
5
Dust Detection System Observation of surfaces of spacecrafts recovered
Example: LDEF (Long Duration Exposure Facility,), EURECA (European Retrievable
Carrier ), SFU (Space Flyer Unit)
G. Drolshagen, ESA/TOS-EMA 21th IADC, 10-13 March 2003, Bangalore, India
High cost Low Earth Orbit only
6
Acoustic Emission Method Acoustic Emission (AE) is an elastic wave motion phenomenon
in a solid. AE occurs when an impact happens on a solid or when
destruction happens in a solid.
Impact
destruction
7
Acoustic Emission Method
Impact position can be detected by solving the following equations.
iei
iiii
tvRR
zyxR
czbyaxR
0
2220
222
S(x, y, z): Impact position
Ti(ai, bi, ci): i th AE sensor position
ve: Wave velocity
ti: Arrival time of a wave at i th AE sensor
z
x
y
S(x, y, z)
T0(a0, b0, c0)
T1(a1, b1, c1)
Ti(ai, bi, ci)
TN(aN, bN, cN)
8
Experiments
Two experiments were performed by free fall. a light gas gun.
Experiments by free fall are in preparation for impacts by a gas gun.
Experiments by a gas gun are representative of impacts in space.
9
Experiments Free fall
type of panel dimensions(mm) projectile
Aluminum alloy panel( A 5052) 150×160×5
A 2017φ1 mm1.4 mg
CFRP layered panel( 0/90, 4 ply) 150×150×0.8
Aluminum honeycomb sandwich panel 150×150×12
Aluminum honeycomb sandwich panel with CFRP face sheets 150×150×10.8
4 different types of panel and 1 type of projectile were used in free fall.
Projectiles were dropped from 380 mm above position of panels.
Impact velocity was about 2.7 m/s.
10
Experiments
Results of experiments by free fall
-5
-4
-3
-2
-1
0
1
2
3
4
5
-50 -30 -10 10 30 50
Time(μs)
Am
plit
ude(V)
AE No.1AE No.2AE No.3AE No.4
Aluminum alloy panel CFRP layered panel
-5
-4
-3
-2
-1
0
1
2
3
4
5
-100 -80 -60 -40 -20 0
Time(μs)
Am
plit
ude (
V)
AE No.1AE No.2AE No.3AE No.4
11
Experiments
Results of experiments by free fall
-5
-4
-3
-2
-1
0
1
2
3
4
5
-50 -30 -10 10 30 50
Time(μs)
Am
plit
ude (
V)
AE No.1AE No.2AE No.3AE No.4
Aluminum honeycomb sandwich panel
Aluminum honeycomb sandwich panel with CFRP face sheets
-5
-4
-3
-2
-1
0
1
2
3
4
5
-150 -130 -110 -90 -70 -50
Time(μs)
Am
plit
ude (
V)
AE No.1AE No.2AE No.3AE No.4
12
Experiments Gas gun
type of panel dimensions(mm) projectile
Aluminum alloy panel( A 5052) 400×200×5
A 2017φ3.175 mm
45 mg
CFRP layered panel( 0/90, 4 ply) 400×200×0.8
Aluminum honeycomb sandwich panel 400×200×12
Aluminum honeycomb sandwich panel with CFRP face sheets 400×200×10.8
4 different types of panel and 1 type of projectile were used in a gas gun.
Impact velocity was about 668.4 m/s. Vacuum level was about 1.0*103 Pa
13
Experiments Results of experiments by a gas gun
-5
-4
-3
-2
-1
0
1
2
3
4
5
-20 -15 -10 -5 0 5 10
Time(μs)
Am
plit
ud
e(V
)
AE No.1AE No.2AE No.3AE No.4
-5
-4
-3
-2
-1
0
1
2
3
4
5
-15 -10 -5 0 5 10 15
Time(μs)
Am
plit
ude (
V)
AE No.1AE No.2AE No.3AE No.4
Aluminum alloy panel CFRP layered panel
14
Experiments
Results of experiments by a gas gun
-5
-4
-3
-2
-1
0
1
2
3
4
5
-10 0 10 20 30 40 50
Time(μs)
Am
plit
ude (
V)
AE No.1AE No.2AE No.3AE No.4
-5
-4
-3
-2
-1
0
1
2
3
4
5
-40 -20 0 20 40 60 80
Time(μs)
Am
plitu
de (
V)
AE No.1AE No.2AE No.3AE No.4
Aluminum honeycomb sandwich panel
Aluminum honeycomb sandwich panel with CFRP face sheets
15
Results compared real impact position with predicted impact
position on experiments by free fall
Real Impact Position Calculated Impact Position Errors
x(mm) y(mm) x(mm) y(mm) Δx(mm) Δy(mm)
0 0 0.7 0.0 0.7 0.0
10 0 22.3 -5.2 12.3 5.2
20 0 26.7 -2.8 6.7 2.8
30 0 35.9 -1.6 5.9 1.6
40 0 42.4 -1.0 2.4 1.0
50 0 64.5 -0.6 14.5 0.6
-10 0 -0.4 0.5 9.6 0.5
-20 0 -22.5 1.4 2.5 1.4
-30 0 -30.9 2.1 0.9 2.1
-40 0 -46.7 -3.0 6.7 3.0
-50 0 -62.9 -2.5 12.9 2.5
-60 0 -66.6 -0.6 6.6 0.6
Aluminum alloy panel
Average of errors 6.8 1.8
Standard deviation 4.5 1.4
16
Results compared real impact position with predicted impact
position on experiments by free fallReal Impact Position Calculated Impact Position Errors
x(mm) y(mm) x(mm) y(mm) Δx(mm) Δy(mm)
0 0 2.1 0.6 2.1 0.6
10 0 3.1 0.3 6.9 0.3
20 0 18.4 1.1 1.6 1.1
30 0 24.7 -11.5 5.3 11.5
40 0 41.5 3.2 1.5 3.2
50 0 61.2 -0.3 11.2 0.3
-10 0 -2.7 -0.2 7.3 0.2
-20 0 -4.9 -2.1 15.1 2.1
-30 0 -44.6 4.3 14.6 4.3
-40 0 -51.8 -3.6 11.8 3.6
-50 0 -62.1 -3.4 12.1 3.4
-60 0 -79.2 5.5 19.2 5.5
CFRP layered panel
Average of errors 9.1 3.0
Standard deviation 5.6 3.1
17
Results compared real impact position with predicted impact
position on experiments by free fall
Real Impact Position Calculated Impact Position Errors
x(mm) y(mm) x(mm) y(mm) Δx(mm) Δy(mm)
0 0 0.5 -0.4 0.5 0.4
10 0 11.0 8.8 1.0 8.8
20 0 17.8 4.0 2.2 4.0
30 0 32.0 -1.2 2.0 1.2
40 0 29.8 0.9 10.2 0.9
50 0 33.3 -2.3 16.7 2.3
-10 0 -3.7 -3.1 6.3 3.1
-20 0 -27.4 -5.8 7.4 5.8
-30 0 -17.9 -2.1 12.1 2.1
-40 0 -44.0 6.9 4.0 6.9
-50 0 -41.3 2.9 8.7 2.9
-60 0 -70.3 11.4 10.3 11.4
Aluminum honeycomb sandwich panel
Average of errors 6.8 4.2
Standard deviation 4.8 3.3
18
Results
compared real impact position with predicted impact position on experiments by free fall
Real Impact Position Calculated Impact Position Errors
x(mm) y(mm) x(mm) y(mm) Δx(mm) Δy(mm)
0 0 0.0 -1.9 0.0 1.9
10 0 0.8 -1.5 9.2 1.5
20 0 26.1 -2.6 6.1 2.6
30 0 29.2 -1.3 0.8 1.3
40 0 35.5 -1.3 4.5 1.3
50 0 61.6 -2.0 11.6 2.0
-10 0 -0.2 -1.9 9.8 1.9
-20 0 -11.7 -2.4 8.3 2.4
-30 0 -25.6 -3.3 4.4 3.3
-40 0 -37.9 -1.8 2.1 1.8
-50 0 -39.1 -9.9 10.9 9.9
-60 0 -53.9 7.7 6.1 7.7
Aluminum honeycomb sandwich panel with CFRP face sheets
Average of errors 6.2 3.1
Standard deviation 3.7 2.6
19
Results Compared real impact position with predicted impact position
on experiments by a gas gun
Real Impact Position Predicted Impact Position Errors
x(mm) y(mm) x(mm) y(mm) Δx(mm) Δy(mm)
-4.9 13.9 0.2 0.0 5.1 13.9
53.8 24.0 56.6 40.5 2.8 16.5
Real Impact Position Predicted Impact Position Errors
x(mm) y(mm) x(mm) y(mm) Δx(mm) Δy(mm)
9.4 -8.2 0.0 -0.1 9.4 8.1
-14.0 8.1 0.0 0.1 14.0 8.0
Aluminum alloy panel
CFRP layered panel
Average of Errors 4.0 15.2
Average of Errors 11.7 8.1
20
Results Compared real impact position with predicted impact position
on experiments by a gas gun
Real Impact Position Predicted Impact Position Errors
x(mm) y(mm) x(mm) y(mm) Δx(mm) Δy(mm)
-56.6 3.6 -3.2 12.4 53.4 8.8
36.1 -4.1 2.5 -3.3 33.5 0.8
Real Impact Position Predicted Impact Position Errors
x(mm) y(mm) x(mm) y(mm) Δx(mm) Δy(mm)
-7.8 14.6 -0.6 4.0 7.2 10.6
Aluminum honeycomb sandwich panel
Aluminum honeycomb sandwich panel with CFRP face sheets
Average of Errors 43.5 4.8
21
Results
Aluminum alloy panelError- 5.7 % of the distance of sensors
CFRP layered panelError- 8.4 % of the distance of sensors
Aluminum honeycomb sandwich panelError- 5.7 % of the distance of sensors
Aluminum honeycomb sandwich panel with CFRP face sheetsError- 7.6 % of the distance of sensors
22
Conclusions
Dust detection system is possible by using AE sensors. It is more difficult to decide the arrival time accurately in
panels using CFRP and honeycomb sandwich. Buffers are needed to relieve the impacts to AE sensors. There are little influence of holes by impacts to detect the
impact points.