Minutes from 29 Mar 2006 SWMD Telephone Meeting
Present: Jonny Smith, Justin Greenhalgh, Nigel Watson
Minutes: Nigel
Notes from previous meeting
- Material damage
- Conclusion
of SLAC damage test work - Justin (for George)
George had studied temperature as function of time over short
period 0.01s to check behaviour using smaller time steps - noted
that ANSYS calculations are cumulative, so uncertainties at very
short time scale will lead to unreliable results at longer
timescales, even if the behaviour looks like aymptotic convergence
to some physical value. Used energy deposition in space from one
of Luis' Fluka simulations at 250 GeV, goal is to determine
appropriate time steps to reduce uncertainties to acceptable
level. Large fluctuations found for time steps 2e-4s, 1.e-4s,
smooth reduction in temperature when steps of 25microsec used.
Due to boundary conditions imposed, the max. temperature rise is
artificially less than expected at long times - heat cannot escape
from the surface of the model. In ESA, only a relatively small
amount of energy could be deposited in the collimator material in
a very small volume, after this has spread even a short distance,
the max. temperature rise would be dramatically reduced. Even
with boundary condition limitations, peak temp. rise of ~250K is
reduced to 50K after 5ms - so conclusion is that 10Hz beam would
not offer a realistic test.
- von
Mises stress for the fully constrained model - Justin (for
George)
Simulation of VM stresses with time, showed clearly stress wave
reflected from surface of volume, not so obvious why stress is
non-zero at small initial times, as definition of VM stress
requires some asymmetry in components resolved along three
orthogonal axes, and initially would expect equal expansion in all
directions. Can be checked by examination of individual stresses
along each axis.> At end of simulation, would be interesting to
see behhaviour at slightly longer time when stress wave re-enters
the initially-heated zone, e.g. additional 8e-12s?
- Wakefield simulations:
GdfidL
output for cylindrically symmetric jaws
- Summary of pbx runs
- Summary of pbxb runs
- Runtime durations
Jonny described the detailed studies he has carried out on
sensitivity of his loss factor simulations to input parameters
such as no. of mesh cells per sigma_z, aspect ratio of the mesh,
and bunch length, using as example the pill box cavity.
Discussed for transverse loss calculation what the appropriate
normalisation is for the case when GdfidL chooses not to carry
out integration along the requested displacement off the symmety
axis - does transverse loss factor (V/pC/m) use distance
*requested* off axis of symmetry, or *actual* distance? Appears
that results are for "requested". Results are found more stable
for larger cells/sigma z, results are stable to within 10%
relative uncertainty using 8 cells/zigma. For mesh aspect ratio,
choice will depend on model being studied to some extent. Aim is
to include ABCI calculation on his parameter sweep comparisons
(already includes analytic calculation) and then continue with
collimators for ESA run - using default 8 cells/sigma z - and
single choice of aspect ratio, and 0.3mm sigma_z. Additional
parameter variations to demonstrate stability around these values
can be studied after baseline predictions have been made. Noted
that collimators 7 and 8 will be different to others having two
different taper angles and collimator 3 will have few different
flat section lengths studied, not expected to be necessary to
include 1m section.
- Analytic calculations - spreadsheet - Nigel
Minor changes to this to include predictions of deflection angles
per unit offset of beam/collimator centre (microrad/mm).
Deflections expected to be substantially smaller than in previous
runs, so need to average over more bunches to achieve good
resolution on kick factors. Needs stability of BPM calibration over
at least the time of a signicant part of the scan. Implication for
scan strategy (e.g. high statistics points throughout collimator
scan, perhaps recalibration, then filling in remaining points?).
- Wire/bench test preparations
Carl had noted yesterday that there was a delay in hardware
fabrication required for the tests, 3-4 weeks.
- Progress for ESA tests
- Arrived safely at SLAC - 21-Mar-2006 - now with vacuum group.
- Sandwich modifications for the new Uk collimators are being
made, Steve Molloy is taking charge of these
- Matlab Reconstruction
code - Nigel (for Luis)
Luis has made a first simulation of the effects of finite BPM
resolution on the measurements, taking BPM z locations from optics
tables (two upstream BPMs, c/o Frank J.), and of six downstream BPMs
from the layout plans (therefore approx. - not from a surveyed
measurement). He has assumed 1 micron rms noise on each BPM, and
with 50 pulses/y position the resolution on kick factor is less
good than expected, for 500/position looks OK, with relative error
on kick factor (of 0.5microrad/mm) of ~10%. For this, a purely
linear dependence on the kick angle as function of y was assumed
for simplicity, this can be made more sophisticated (e.g. cubic
near collimator wall) at later stage.
Next steps are to include beam jitter, implemented as coherent
noise assigned to all BPMs.
- Travellers for ESA run
Please confirm travel plans with Mike Woods, cc: Nigel if you
have not done so already. Also, could people travelling to SLAC
for the run, please try to phone in to the ESA Monday
meetings for the next few weeks if they do not do so already.
- Future plans
There will be a (closed, management/WP/task leaders) UK meeting on
3-Apr to discuss aims for post-Apr-2007 period, with open meeting
at Manchester on 24-Apr.
- Next meeting: date to be fixed outside meeting, suggest
Thu. 20-Apr