rf tutorial g burt. tm 010 monopole mode e h beam z 0 =377 ohms
TRANSCRIPT
![Page 1: RF Tutorial G Burt. TM 010 Monopole Mode E H Beam Z 0 =377 Ohms](https://reader036.vdocuments.us/reader036/viewer/2022083009/5697bf9e1a28abf838c947b7/html5/thumbnails/1.jpg)
RF Tutorial
G Burt
![Page 2: RF Tutorial G Burt. TM 010 Monopole Mode E H Beam Z 0 =377 Ohms](https://reader036.vdocuments.us/reader036/viewer/2022083009/5697bf9e1a28abf838c947b7/html5/thumbnails/2.jpg)
TM010 Monopole Mode
0 0
0 10
2.405
0
0
2.405
0
0
i tz
z
r
i t
r
rE E J e
R
H
H
i rH E J e
Z R
E
E
E
H
Beam
Z0=377 Ohms
![Page 3: RF Tutorial G Burt. TM 010 Monopole Mode E H Beam Z 0 =377 Ohms](https://reader036.vdocuments.us/reader036/viewer/2022083009/5697bf9e1a28abf838c947b7/html5/thumbnails/3.jpg)
Transit time factor• An electron travelling close to the speed
of light traverses through a cavity. During its transit it sees a time varying electric field. If we use the voltage as complex, the maximum possible energy gain is given by the magnitude,
• Where T is the transit time factor given by
• For a gap length, g.• For a given Voltage (=E0L) it is clear that
we get maximum energy gain for a small gap.
/ 2
/0
/ 2
,L
i z cz
L
E eV e E z t e dz E LT
/ 2
/
/ 2
/ 2
/ 2
, sin
,
Li z c
z
L
L
z
L
gE z t e dz
Tg
E z t dz
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 10
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
g/bl
Tra
nsi
t ti
me
fact
or,
T
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Transit time factor• The maximum energy gain is hence
• Considering the cavity length is g=l/4
0
sin g
E eV E Lg
0
sin 4E eV E
![Page 5: RF Tutorial G Burt. TM 010 Monopole Mode E H Beam Z 0 =377 Ohms](https://reader036.vdocuments.us/reader036/viewer/2022083009/5697bf9e1a28abf838c947b7/html5/thumbnails/5.jpg)
Shunt Impedance
• Another useful definition is the shunt impedance,
• This quantity is useful for equivalent circuits as it relates the voltage in the circuit (cavity) to the power dissipated in the resistor (cavity walls).
• Shunt Impedance is also important as it is related to the power induced in the mode by the beam (important for unwanted cavity modes)
21
2c
sc
VR
P
![Page 6: RF Tutorial G Burt. TM 010 Monopole Mode E H Beam Z 0 =377 Ohms](https://reader036.vdocuments.us/reader036/viewer/2022083009/5697bf9e1a28abf838c947b7/html5/thumbnails/6.jpg)
TM010 Shunt Impedance
0
0 10
sin 4
2.405
cV E
i rH E J
Z R
2
220
, 120
220
, 120
220
120
1
2
2.4052
2.405
2.405
c surface
c ends surface
c walls surface
c surface
P R H dS
E rP R r J dr
Z R
EP RL R J
Z
EP R R L R J
Z
2
231
sin 4
/ 4 2.405s
surface
RR R R J
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Radius
• For a pillbox TM010 mode the radius is given by
• k=w/c• R=2.4/k=2.4l/2p
2
231
sin 4
2.405 2.405/ 4 2.405
2 2
s
surface
RR J
![Page 8: RF Tutorial G Burt. TM 010 Monopole Mode E H Beam Z 0 =377 Ohms](https://reader036.vdocuments.us/reader036/viewer/2022083009/5697bf9e1a28abf838c947b7/html5/thumbnails/8.jpg)
• What is the maximum gradient of a 100 cell 12 GHz structure driven by a 50 MW klystron (assume pillbox parameters)
• Rs=5E4/Rsurf
• For 100 cells
2Rsurf
4 46
8 7
5 10 2 5 10 21.25 10
2 (12 )(1.7 10 )(4 10 )sR
GHz
8(100 ) 100* 1.25 10s cells sR R
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• What is the maximum gradient of a 100 cell 12 GHz structure driven by a 50 MW klystron (assume pillbox parameters)
• V for 50 MW
• Gradient is V/L
7 8 6(100 ) 5 10 1.25 10 78.8 10s cellsV PR
6679 10
63 100.0125 100
VGradient
L
= 63 MV/m