Prototype and Design of High-Speed X-Ray Chopper

Slides:



Advertisements
Similar presentations
Ian Bailey Cockcroft Institute/ Lancaster University October 30 th, 2009 Baseline Positron Source Target Experiment Update.
Advertisements

QA for the Fibre Tracker 28 October 2004Brunel QA for fibre bundling Dr Paul Kyberd and Dr Peter Hobson School of Engineering & Design Brunel University,
III. Results and Discussion In scanning laser microscopy, the detected voltage signal  V(x,y) is given by where j b (x,y) is the local current density,
Construction of a Laser Frequency Stabilization System for a Magneto Optical Trap Talia Martin and Dr. Edward Deveney Department of Physics, Bridgewater.
Sci 701 Unit 6 As learned in Unit 5: Speed, Power, Torque, and DC Motors, a motor can generate a set amount of power. Introduction to Gears Since there.
Unit 4: Electromechanical drive systems An Introduction to Mechanical Engineering: Part Two Electromechanical drive systems Learning summary By the end.
AAC February 4-6, 2003 Protons on Target Ioanis Kourbanis MI/Beams.
STEPPER MOTORS Name: Mr.R.Anandaraj Designation: Associate. Professor Department: Electrical and Electronics Engineering Subject code :EC 6252 Year: II.
HIRADMAT tungsten powder experiment Presented by Ottone Caretta Presented by Ottone Caretta
INTRODUCTION TO ROBOTICS Part 3: Propulsion System Robotics and Automation Copyright © Texas Education Agency, All rights reserved. 1.
2/25-26 Obj: I can apply concepts of physics – energy, work, and efficiency--- to describe motion. What you should have in the ENB: Write down the first.
AirSpeed Calibration Facility by using LDV and A Wind Tunnel at CMS
1 BROOKHAVEN SCIENCE ASSOCIATES Beam Stability Overview NSLS-II CFAC Meeting May 8, 2007 S. Krinsky.
CNC FEED DRIVES Akhil Krishnan G M.Tech 1. CONTENTS 1.Introduction 2.Requirements of CNC feed drives 3.Servo motor 3.1 Servo drive control 3.2 Components.
CNC FEED DRIVES.
The Electromagnetic Spectrum High Harmonic Generation
Jonathan Donkers1, Lin Zhang1+
Measuring the Thickness of Cryosheet Jets
Madhu Karra1, Jason Koglin1,2
A New type of Kapton® Window Holder
Image Processing For Soft X-Ray Self-Seeding
UNIT-3 ADVANCES IN METROLOGY
Characterizing Optics with White-Light Interferometry
Matter in Extreme Conditions at LCLS:
Kevin Shimbo1, Matt Hayes+
X-Ray Shielding Introduction Application Research Conclusions
Crystallography images
Hutch 4 (XCS) Laser System
Anomaly Detection LCLS data: Introduction Research Conclusion
MAKING WAY FOR LCLS II HERRIOTT CELL IGNIS THE NEED FOR LCLS-II
A remote EPICS monitoring tool
EASE: Alert Management
Designing and Prototyping Optics Table and Shelves
Odu/slac rf-dipole prototype
Managing Diffraction Beam
Effects of Wrapping Vacuum
Scintillation Material Encapsulation Fixture
LCLS CXI Sample Chambers and Engineering Solutions
Values to Normalize Data
LAMP Vacuum System Documentation
Your Name, Elias Catalano, Robert Sublett, Robin Curtis
Determining a Detector’s Saturation Threshold
HXRSD Helium Enclosure
Crystallography Labeling Using Machine Learning
IT Inventory and Optimization
Structural study of soluble ammonia monooxygenase
Creation and development of a PRP database
Electro Optic Sampling of Ultrashort Mid-IR/THz Pulses
Margaret Koulikova1, William Colocho+
POWER AMPLIFIERS.
Analytical Solutions for Heat Distribution in KB Mirror Systems
Repeatability Test of Attocube Piezo Stages
Analytical Solutions for Temperature
Barron Montgomery1,2, Christopher O’Grady2, Chuck Yoon2, Mark Hunter2+
P08310 PNEUMATICALLY CONTROLLED AUTOMATED SHIFTING SYSTEM FOR A POLARIS OUTLAW / Polaris Industries - Joel Notaro (Sponsor) Professor.
Elizabeth Van Campen, Barrack Obama2, Stephen Curry1,2, Steve Kerr2+
Advanced Methods of Klystron Phasing
Ryan Dudschus, Alex Wallace, Zachary Lentz
Jennifer Hoover1, William Colocho2
Interference Introduction to Optics Coherent source
Amplifiers Classes Electronics-II
X-Ray Spectrometry Using Cauchois Geometry For Temperature Diagnostics
Redesigning of The SED Calendars
Automatic compression control for the LCLS injector laser
Amplifiers Classes Electronics-II
Russell Edmonds1, Matt Hayes2+ 1LCLS Summer Research Intern
Title of Your Poster Introduction Research Conclusions Acknowledgments
Electrons Thermionic Emission
Reconstruction algorithms Challenges & Future work
P08310 PNEUMATICALLY CONTROLLED AUTOMATED SHIFTING SYSTEM FOR A POLARIS OUTLAW / Polaris Industries - Joel Notaro (Sponsor) Professor.
Presentation transcript:

Prototype and Design of High-Speed X-Ray Chopper William Choi1, Rebecca Armenta2+ 1Mechanical and Aerospace Engineering Department, University of California, Los Angeles, 405 Hilgard Ave, Los Angeles, CA 90095, USA 2Linac Coherent Light Source, SLAC National Accelerator Laboratory, 2575 Sand Hill Road, Menlo Park, CA 94025, USA. +Contact: rebeccaa@slac.stanford.edu Scoping Out the Mission On the Chopping Board Sizing the Motor The LCLS Detector Group has been tasked to test new detectors for LCLS II. The group has a continuous x-ray source at its disposal, but LCLS II detectors are designed to operate with the pulsed x-ray produced by the linac. In order to yield meaningful results, the detectors require a chopper to mechanically parse the incident x-ray beam into single microsecond pulses. Considering vacuum rotary motion feedthroughs, physical constraints, and detector photosensitivity, the goal of this project is to prototype and design an x-ray chopper. Keywords: continuous, pulsed, chopper, microsecond At a given rotation speed, the tunnel chopper experiences greater damping forces (ie: bearing friction and air drag) and demands greater motor torque than does the slots chopper. Accordingly, the new motor was sized to the demands of the tunnel chopper. Figure 4. Motor Sizing Curve. Displayed above is the torque-speed curve for the motor used in the chopper prototype. The gray stall torque curves were determined empirically, while the red theoretical curve was determined using motor specifications. The orange curve represents a viable upsize option. Slots Tunnel Design Considerations Physical Size: The chopper should be no larger than 6 to 8 inches in diameter in order to fit inside a reasonably sized vacuum chamber. Vacuum Rotary Motion Feedthroughs: Commercially available ferromagnetic fluid feedthroughs can deliver up to 10,000 RPM into vacuum. Gear friction outgasses and contaminates vacuum. Source Beam Collimation: The diameter of the incident beam will be much larger than the desired aperture width. 1.95 Chopper Radius at Aperture (in) 2.00 0.03 Aperture Radius (in) 12 Voltage (V) 9800 Motor Speed (RPM) 6400 16.4 Repetition Rate (kHz) 6.4 58 Predicted Pulse Width (µs) 38 42 Empirical Pulse Width (µs) Large pulse width Easy to machine East to mount in vacuum Low absorption efficiency Light and thin Defining Characteristics Small pulse width More difficult to machine More difficult to mount High absorption efficiency Heavy and thick Looking Ahead As of the last completed design revision, the tunnel chopper has delivered a 42 microseconds pulse width, with the capability of going as low as 28 microseconds. The next revision features smaller apertures and a new motor, with a goal of achieving a 19 microseconds pulse width. This prototype process has illuminated many design needs in regard to the ultimate mission of providing a chopper to pulse a continuous x-ray. As one progresses into the final design phase, one might consider the following improvements to the system: Goal The goal of the chopper is to reduce the continuous x-ray source into 1 µs (0.000001 s) pulses at 10 kHz, as shown in the figure below. Figure 1. Ideal Signal. Displayed above is the desired pattern of emitted x-ray light. High signals represent transmittance of x-ray light, while low signals represent blockage. This waveform can be simulated with a laser diode and an oscilloscope. Pulse Width < 1 µs Areas for Improvement Mitigation Speed Control Implement closed-loop feedback from photodiode using Arduino Laser, Collimator, and Chopper Alignment Install bellows and stages Vacuum Rotary Motion Feedthrough Speed Research Julich technology Chopper Size Increase radius to 3 inches Collimation Research affect on light intensity Resonant Frequency Vibrations Install physical supports or damping mechanism Chopper Stability Determine vibration in horizontal plane using Keyence laser displacement sensor Pulse Width Research multi-part chopper systems Period = 100 µs (10 kHz) Figure 3. Chopper Design Comparison. The geometry of the tunnel chopper allows it to parse incoming light into pulse widths half as long as those produced by the slots chopper. Below each model is the waveform of the oscilloscope signal at the rated motor voltage. Printing a Prototype The proof of concept of a chopper can be demonstrated using a functional prototype. The prototype makes use of a hobby motor, 3-D printed parts, Thorlabs laser optics, and a Hamamatsu photodiode. Figure 2 depicts the latest design of the chopper prototype. 3-D printed parts are rendered in color. Figure 2. Prototype Assembly. Depicted above is the Solid Edge assembly of the chopper prototype. The laser diode (right), secured in a kinematic mount, emits a beam through the red collimator. The beam is then parsed by the rotating chopper (center) before striking the photodiode (left) in pulses. The motor (hidden) is driven by a power supply, through an Arduino microcontroller. Note that the model illustrates a moment of peak light intensity incident upon the photodiode. Microcontroller DC Motor Tunnel Chopper Photodiode Laser (Class 2) Oscilloscope Collimator Figure 4. Final Design Considerations. The table above lists the topics to be addressed in the final design. Acknowledgments Power Alan Fry for offering me this internship at LCLS Rebecca Armenta for mentorship Kazutaka Nakahara for addition guidance LCLS Detector Group: Mark McKelvey, Rebecca Armenta, Kazutaka Nakahara, and Philip Hart for providing lab space Greene Scholars and SAGE for the opportunity to concurrently volunteer and learn skills relevant to my project Use of the Linac Coherent Light Source (LCLS), SLAC National Accelerator Laboratory, is supported by the U.S. Department of Energy, Office of Science, Office of Basic Energy Sciences under Contract No. DE-AC02-76SF00515. Motor Mount Date: 08/03/2018