Fast Current Diagnostic Techniques for Linear Pulsed Beams

Fast Current Diagnostic of Linear Pulsed
Beams
 
Dipartimento di Matematica e Fisica
“Ennio De Giorgi”
 
Vincenzo Nassisi, Luigi Monteduro,
Daniela Manno, Antonio Serra
5-7/7/2017
Plasma Physics by Laser and Applications
2017, Messina-I
-
 
CYLINDRICAL beams and LINEAR beams
-
 
Evolution of Rogowski coil
-
 
Exploiting Rogowski coil for linear  structure
-
 
Apparatus for the calibration
-
  
Application to a plane line
-
  
Results 
 
-
 Conclusion
Outline of talk:
5-7/7/2017
Plasma Physics by Laser and Applications
2017, Messina-I
Cylindrical
Cylindrical
 and Linear 
 and Linear 
beam
beam
 
Particles
Particles
5-7/7/2017
Plasma Physics by Laser and Applications
2017, Messina-I
Cylindrical
Cylindrical
 
 
beam
beam
 
Fig. 1: Electrical circuit of a toroidal Rogowski
coil with the input current in the centre.
5-7/7/2017
Plasma Physics by Laser and Applications
2017, Messina-I
planar currents fluxing in a metallic sheet.
Fig. 2: Sketch of a Rogowski coil
employed in a planar conductor
Plane 
Plane 
 
 
beam
beam
5-7/7/2017
Plasma Physics by Laser and Applications
2017, Messina-I
Plane current fluxing in two
Plane current fluxing in two
metallic sheet
metallic sheet
.
Fig. 3: Sketch of a Rogowski coil employed
between two plane conductors.
5-7/7/2017
Plasma Physics by Laser and Applications
2017, Messina-I
input
output
R
o
g
o
w
s
k
i
 
c
o
i
l
 
a
s
 
d
i
s
t
r
i
b
u
t
e
d
 
e
l
e
m
e
n
t
s
Fig. 4: Sketch of a Rogowski coil employed in a metallic box
Fig. 5: Electric sketch of a Rogowski coil closed into the metallic box
5-7/7/2017
Plasma Physics by Laser and Applications
2017, Messina-I
R
o
g
o
w
s
k
i
 
c
o
i
l
 
a
s
 
d
i
s
t
r
i
b
u
t
e
d
 
e
l
e
m
e
n
t
s
Applying the Kirchhoff’s equations, the 
differential of voltage and
current for every cell to differential of position depend through the
 following equations. 
 Z=R+Ldi/dt+R and Y=G+ C      .
5-7/7/2017
Plasma Physics by Laser and Applications
2017, Messina-I
R
o
g
o
w
s
k
i
 
c
o
i
l
-
I
n
f
l
u
e
n
c
e
 
o
f
 
c
o
i
l
 
r
e
s
i
s
t
a
n
c
e
5-7/7/2017
Plasma Physics by Laser and Applications
2017, Messina-I
But Ls depend by the slits, the
response depends on the slit
5-7/7/2017
Plasma Physics by Laser and Applications
2017, Messina-I
Materials and calibration
Fig. Double lines of 100
.
5-7/7/2017
Plasma Physics by Laser and Applications
2017, Messina-I
Experimental resutls
Time scale 500 ps
5-7/7/2017
Plasma Physics by Laser and Applications
2017, Messina-I
Experimental resutls
The attenuation was 675 A/V
Risetime input 400 ps
Risetime response 500 ps
Thanks
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Explore the advancements in plasma physics and beam diagnostics presented at the Plasma Physics by Laser and Applications conference in Messina. Through detailed talks and images, the evolution of Rogowski coils for linear structures, apparatus calibration, and results are showcased. Discover the application of Rogowski coils in analyzing cylindrical and linear beam particles, as well as tracking current flux in metallic sheets with innovative setups. The use of distributed Rogowski coils in metallic boxes is also discussed for efficient current monitoring.

  • Plasma Physics
  • Beam Diagnostics
  • Rogowski Coils
  • Current Monitoring
  • Metal Sheets

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  1. aboratorio di lettronica pplicata e trumentazione Dipartimento di Matematica e Fisica Ennio De Giorgi Fast Current Diagnostic of Linear Pulsed Beams Vincenzo Nassisi, Luigi Monteduro, Daniela Manno, Antonio Serra Plasma Physics by Laser and Applications 2017, Messina-I 5-7/7/2017

  2. Outline of talk: - CYLINDRICAL beams and LINEAR beams - Evolution of Rogowski coil - Exploiting Rogowski coil for linear structure - Apparatus for the calibration - Application to a plane line - Results - Conclusion Plasma Physics by Laser and Applications 2017, Messina-I 5-7/7/2017

  3. Cylindrical and Linear beam Particles Particles Plasma Physics by Laser and Applications 2017, Messina-I 5-7/7/2017

  4. Cylindrical beam ???? ?? ?0(?) = ?? + ????(?) ???(?)?? Fig. 1: Electrical circuit of a toroidal Rogowski coil with the input current in the centre. ?= ????(?) + ???(p) ?? ?? ??(?) =?? ?? ? ? ? Now, hypothesizing a Heaviside function as current signal, i.e. ?(?) = ???(?), its transform is ??(?) = ???. Then the real output current results ??(?) =?? ? ? ? ??? ? ??? ?????? Plasma Physics by Laser and Applications 2017, Messina-I 5-7/7/2017

  5. Plane beam planar currents fluxing in a metallic sheet. ? 2? ?? ? ?? Fig. 2: Sketch of a Rogowski coil employed in a planar conductor ?0? = ??? ? ???? ?? 1 ??? ??? = 2? ??(?) =?? 2? ? ??? ? ??? ?????? ?? ? ) ) ??(? ?(? =1 ?? ?? +?? ? ?? Plasma Physics by Laser and Applications 2017, Messina-I 5-7/7/2017

  6. Plane current fluxing in two metallic sheet. ? ???? ?? ??? =1 ??? ? Fig. 3: Sketch of a Rogowski coil employed between two plane conductors. ??? =1 ? ???? ? ??? ? ??? ?????? ? ) ) ??(? ?(? =1 ? ? ?? input ?? +?? ? ?? output Plasma Physics by Laser and Applications 2017, Messina-I 5-7/7/2017

  7. Rogowski coil as distributed elements Fig. 4: Sketch of a Rogowski coil employed in a metallic box Fig. 5: Electric sketch of a Rogowski coil closed into the metallic box Plasma Physics by Laser and Applications 2017, Messina-I 5-7/7/2017

  8. Rogowski coil as distributed elements Applying the Kirchhoff s equations, the differential of voltage and current for every cell to differential of position depend through the ?? following equations. Z=R+Ldi/dt+R and Y=G+ C . ???(?,?) ?? = ? ?,? ???,? ?(?,?) ) ???(?,? ?? = ? ?,? ???,? Due to the slit Z and Y assume the following form: ? ??+ ??? ? ??+ 1 ? = ? + ? ? ??? ?? ? = ? ? ? ? ?? . . Plasma Physics by Laser and Applications 2017, Messina-I 5-7/7/2017

  9. Rogowski coil-Influence of coil resistance Considering R 0, 1 ?? 0 the response is 1 ???,? ? ? ?? ?? + ??? But Ls depend by the slits, the response depends on the slit Plasma Physics by Laser and Applications 2017, Messina-I 5-7/7/2017

  10. Materials and calibration The coil was 4 mm in diameter and 27 mm long. The wire has a 0.11 ?? in diameter which provides a maximum value of turn density of 80 ?????/?? with a total of 216 turns. Fig. Double lines of 100 . Plasma Physics by Laser and Applications 2017, Messina-I 5-7/7/2017

  11. Experimental resutls The input pulse was 80 ns long. The response c oil was 4 mm in diameter and 27 mm long. The wire has a 0.11 ?? in diameter which provides a maximum value of turn density of 80 ?????/?? with a total of 216 turns. Time scale 500 ps Plasma Physics by Laser and Applications 2017, Messina-I 5-7/7/2017

  12. Experimental resutls The attenuation was 675 A/V Risetime input 400 ps Risetime response 500 ps Thanks Plasma Physics by Laser and Applications 2017, Messina-I 5-7/7/2017

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