Modelling the Skew Quadrupole Component

-- Effects of Coil Offsets and Widening --



Special Meeting on Production of 8-Pole Wigglers

17 November 2003

This talk briefly reviews the prior studies of coil offsets, which were primarily for the 7-pole design, then presents modelling results for an 8-pole wiggler where alternate upper 20-cm coils are offset in a zig-zag pattern, showing that this effect results in a large first integral which is not observed in the measurements. Then a model where the two same-polarity upper 20-cm poles are widened maintaining left/right symmetry, as suggested by Eric Smith (see meeting of 10 Nov 03), is presented. This model appears promising as an explanation of the measured skew quad component in the present wiggler construction. Finally, a model of the warm test set-up now in use for coil production provides information on the acceptance criteria presently applied to coil production relative to the magnitude of the observed skew quad components in the measured field integrals. Postscript files are also available via the links below.

  1. The effect of coil offsets has been studied in the past ( 25Oct02, 1Nov02, 22Nov02, 6Dec02, 10Jan03, 31Jan03, 7Feb03 ), but primarily for the 7-pole design, since the 8-pole designs did not show big skew quad components until recently. At that time, coils were always offset horizontally, breaking the left/right symmetry in a way thought to be necessary to generate the skew quad component. They were simultaneously widened by the amount needed to avoid overlapping the coil with the pole steel. Modelling a single pole offset by 50 mils in wiggler Nr 2 shows that the first integral of the horizontal field component Bx does depend on X, but not as linearly as the measurements show, and that 50 mils is not sufficient to generate the observed slope. A model which used this method to incorporate the coil offsets measured during construction of Wiggler Nr 2 proved that this approach could not account for the large skew quad component measured at the time. Note also that the combined effect of all the offsets exhibits the same curvature in the dependence of the integral on X as shown by the single-coil offset, a characteristic which is not observed in the measurements of the field integrals. For this reason, this line of investigation was abandoned. However, this is only one way of accounting for the measured coil positions. Since the coil position measurement is simply the distance between the outer end of the coil relative to the steel on both sides, it does not specify if these deformations are due to an offset or a widening. The modelling of the 7-pole wiggler chose to subtract the left and right measured coil positions and widen AND shift the coil accordingly. Eric Smith has recently suggested that a symmetric widening of the coils will yield a skew quad effect, and this is verified in the full 8-pole wiggler model below. The above modelling assumption for the 7-pole models would have resulted in no modification of the wiggler field for such coil positioning, since it is sensitive only to left/right asymmetries.

  2. The next four slides show the results of a model in which the four upper 20-cm coils of the 8-pole wiggler are offset and widened by 1.5 mm in a zig-zag pattern in the manner used to model the 7-pole coil offsets. (In this picture, the pattern is seen as almost imperceptible gaps between the coils and the steel on alternating sides of the poles.) The integral of Bx shows that this magnitude of offset generates a large integral at X=0, as well as a quadratic symmetric dependence on X rather than linear, both in contradiction with measurement. Also shown are the integrals and horizontal uniformity of the vertical component of the field.

  3. The model in which two alternate upper 20-cm coils are simply widened by 1.5 mm in the horizontal direction with no offset shows an integral of the horizontal field component which is remarkably similar to the measured integral. It rises roughly linearly with X, and is antisymmetric around X=0. The magnitude of the slope for the 1.5 mm widening of these two poles is about 3/4 of the slope observed for Wiggler Nr 2. Also similar to measurement is the integral of the vertical component, which is about 8 gauss-meters nearly independent of X. The horizontal uniformity of the vertical component remains within specification (3 per mil) and exhibits the left/right symmetry of the model, incontrast to the antisymmetry resulting from coil offsets.

  4. Coil deformations of this type should be detected in the warm single-pole test, which has also been modelled. Measurements are available for the Z-dependence of the integral of the vertical component over X. Comparison of the undeformed coil with the coil widened by 1.5 mm shows that a change in the integral of about 10 gauss-meters can be expected. Sasha reported in this meeting that this corresponds to an acceptance criterion (dN = 1 unit) in his measurement apparatus of about 0.25 mm in the width of the coil. The skew quad component measured for Wiggler Nr 9 is 1.2 gauss-m/cm. The model with the two coils widened by 1.5 mm gives a slope of 1.4 gauss-m/cm (see above). So an unfortunate coincidence of (1.5/0.25) * 1.2 / (1.4/2) = 10 poles, each providing 0.25-mm worth of widening could produce the observed skew quad component in Wiggler Nr 9. From this point of view, the acceptance criterion dN=1 appears marginal.



Creation date: 11/18/03.