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A PRELIMINARY TEST ON THE FEASIBILITY OF LOCATING … · Luigi Sambuelli – DIATI – POLITECNICO...

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Luigi Sambuelli DIATI POLITECNICO DI TORINO Stefano Gallinaro ST-POLITO S.c.ar.l. Michelangelo Grosso ST-POLITO S.c.ar.l. A PRELIMINARY TEST ON THE FEASIBILITY OF LOCATING AN IRON RESTORATION PIN IN A STATUE BY MEASURING THE TMF ANOMALY WITH A TRIAXIAL MEMS MAGNETOMETER
Transcript

Luigi Sambuelli – DIATI – POLITECNICO DI TORINO Stefano Gallinaro – ST-POLITO S.c.ar.l. Michelangelo Grosso – ST-POLITO S.c.ar.l.

A PRELIMINARY TEST ON THE FEASIBILITY OF LOCATING AN IRON RESTORATION PIN IN A

STATUE BY MEASURING THE TMF ANOMALY WITH A TRIAXIAL MEMS MAGNETOMETER

2 Sambuelli, Gallinaro, Grosso GNGTS 2013

Sometimes ancient statue restoration works, carried out during the Renaissance, were done using iron pins inserted in the stone and today invisible.

Archaeologist‘s demands can be more complex than simply stating the presence or not of a pin. A pin located out of the axis, obliquely, within an arm, a leg, a neck, can seriously compromise the safe moving of the artifact.

To estimate the location and the length of an iron pin, at a satisfying approximation level, is a challenge for today’s NDT and micro-geophysics techniques.

3 Sambuelli, Gallinaro, Grosso GNGTS 2013

The “restored arm” analogue model. A 18 cm high cylinder of bioclastite having a diameter of 10 cm. An iron pin (9 cm long, 5 mm diameter) has been inserted and cemented obliquely and out of the sample axis

4 Sambuelli, Gallinaro, Grosso GNGTS 2013

X-ray scans of the sample at the maximum intensity and maximum exposition time available with a veterinary apparatus

5 Sambuelli, Gallinaro, Grosso GNGTS 2013

STMicroelectronics LSM303DLHC 3D Accelerometer and 3D magnetometer module

Magnetic full-scale selectable from 130,000 to 810,000 nT Maximum sensitivity of 90 nT/digit Digital output Size: 3x5x1mm – Power consumption: <400 μW.

6 Sambuelli, Gallinaro, Grosso GNGTS 2013

Sketch of the experimental setup. A vertical scanning arm and a rotating platform allow for measuring the three components over the whole lateral surface of the

sample.

7 Sambuelli, Gallinaro, Grosso GNGTS 2013

Actual realization: vertical scan 1 cm; radial scan 10°.

Measuring on the sample with no pin

Each component at each point measured 50 times at 50 Hz

0

5

10

15

20

25

30

35

40

0 50 100 150 200 250 300 350

Fie

ld [nT

]

Rotation angle [°]

V st. dev of the mean

R st. dev of the mean

T st. dev. Of the mean

Standard deviations of the means of the measured three components at 20 cm of elevation from the rotating platform

8 Sambuelli, Gallinaro, Grosso GNGTS 2013

0

10

20

30

40

50

60

70

80

0 10 20 30 40 50

Stan

dar

d d

evia

tio

n o

f th

e m

ean

[n

T]

Number of samples

Evolution of the standard deviation of the mean. Taking 50 samples a fairly stable value is obtained

9 Sambuelli, Gallinaro, Grosso GNGTS 2013

-40000

-30000

-20000

-10000

0

10000

20000

30000

40000

50000

60000

70000

0 50 100 150 200 250 300 350

Fie

ld [nT

]

Rotation angle [°]

V R

T TMF

Mean values of the measured three components and the modulus at 20 cm of elevation from the rotating platform

No Pin Pin

10 Sambuelli, Gallinaro, Grosso GNGTS 2013

11 Sambuelli, Gallinaro, Grosso GNGTS 2013

bottom

up

Radial components at increasing height

12 Sambuelli, Gallinaro, Grosso GNGTS 2013

Rough location of pin ends from raw radial components

No Pin Pin

13 Sambuelli, Gallinaro, Grosso GNGTS 2013

Vertical component

14 Sambuelli, Gallinaro, Grosso GNGTS 2013

Tangential component

No Pin Pin

15 Sambuelli, Gallinaro, Grosso GNGTS 2013

Radial component

No Pin Pin

16 Sambuelli, Gallinaro, Grosso GNGTS 2013

Modulus

No Pin Pin

17 Sambuelli, Gallinaro, Grosso GNGTS 2013

On summary …….

In spite of the magnetically noisy environment (that however is likely similar to the one in a museum room) even a vectorial raw data representation gives some information on location and length of the iron pin. It must be kept in mind that the results do not represent the magnetic field due to the pin on the surface of the sample.

Other acquisition procedures, such as gradient or gradient tensor data gathering, would allow for a greater deal of information.

On purpose design algorithm for modeling the anomaly field of an iron pin would allow the making up of an inversion, so that the pin location would be less qualitative.

ACKNOWLEDGEMENTS ST-Microelectronics for providing the MEMS sensors and the data acquisition circuitry. Diego Franco for precisely rotating many many many times the sample platform.

18 Sambuelli, Gallinaro, Grosso GNGTS 2013


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