Figure 16.2 has been provided by Steve Wesseln (Fermilab), version from the 15
June 2009.
Figure 16.2:
Dipoles hard edge coordinates for NML compressor lattice
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Table 16.3 reference the coordinates of the dipoles where the origin is taken at the cathode. See figure 3 for convention of notations. The column
and
corresponds to the real geometry(cf figure 16.2) expressed with respect to the entrance point in the first dipole. Nevertheless, in previous simulations from Yin-e Sun[41] a dipole length of 230 mm has been used. We thus add an offset of
mm to the longitudinal coordinate to satisfy this condition. The center of the first dipole being at
m, we write the final coordinates with respect to the cathod in the last column of the table.
Table 16.3:
Dipoles hard edge coordinates in mm for NML compressor
Point |
x |
z |
z dz] |
z+dz+z |
D11 |
-240 |
0 |
-15 |
11650.5 |
D21 |
240 |
0 |
-15 |
11650.5 |
D31 |
-240 |
200 |
215 |
11880.5 |
D41 |
240 |
200 |
215 |
11880.5 |
I1 |
0 |
0 |
-15 |
11650.5 |
O1 |
-32.49 |
200 |
215 |
11880.5 |
D12 |
-527.64 |
885.25 |
870.25 |
12535.75 |
D22 |
-47.64 |
885.25 |
870.25 |
12535.75 |
D32 |
-527.64 |
1085.25 |
1100.25 |
12765.75 |
D42 |
-47.64 |
1085.25 |
1100.25 |
12765.75 |
I2 |
-255.14 |
885.25 |
870.25 |
12535.75 |
O2 |
-287.64 |
1085.25 |
1100.25 |
12765.75 |
D13 |
-527.64 |
1905.09 |
1890.09 |
13555.59 |
D23 |
-47.64 |
1905.09 |
1890.09 |
13555.59 |
D33 |
-527.64 |
2105.09 |
2120.09 |
13785.59 |
D43 |
-47.64 |
2105.09 |
2120.09 |
13785.59 |
I3 |
-287.64 |
1905.09 |
1890.09 |
13555.59 |
O3 |
-255.15 |
2105.09 |
2120.09 |
13785.59 |
D14 |
-240 |
2790.34 |
2775.34 |
14440.84 |
D24 |
240 |
2790.34 |
2775.34 |
14440.84 |
D34 |
-240 |
2990.34 |
3005.34 |
14670.84 |
D44 |
240 |
2990.34 |
3005.34 |
14670.84 |
I4 |
-32.49 |
2790.34 |
2775.34 |
11665.5 |
O4 |
0 |
2990.34 |
3005.34 |
11665.5 |
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