Full Mission Simulation Test Report Cajun Probe University of Louisiana at Lafayette Mark Roberts 5.12.2010.

Slides:



Advertisements
Similar presentations
General Characteristics of Gas Detectors
Advertisements

Radiation Detection ionization chambers (dosimeters, pulse chambers, particle track chambers) scintillation detectors semiconductor detectors photographic.
P2 Controlled Assessment
Effects of an Electric Current and Domestic Circuits Chapter 24.
Chapter 16 Section 1 Kinetic Theory.
GM COUNTER.
Geiger-Muller detector and Ionization chamber
U N I V E R S I T Y L a f a y e t t e OF LOUISIANA RockSat 2010 Team CajunSat Mark Roberts Dr. Andy Hollerman Department of Physics University of Louisiana.
Radiation Detectors / Particle Detectors
PH 0101 UNIT 4 LECTURE 81 LIQUEFACTION OF NITROGEN LIQUEFACTION OF OXYGEN LIQUEFACTION OF AIR ADIABATIC DEMAGNETISATION.
Rocket Investigation D. Crowley, Rocket Investigation Your task is to investigate what affects the maximum altitude a water rocket can reach As.
Lecture 9: D/A and A/D Converters
Capacitors Physics 2415 Lecture 8 Michael Fowler, UVa.
Capacitance and Dielectrics AP Physics C. Applications of Electric Potential Is there any way we can use a set of plates with an electric field? YES!
Project Summary. Mission Statement To develop a Volumetric Flow Sensor to measure the volume of gas flowing through a quadrant and into the combustion.
Team 7, Final Presentation December 1, Mission Overview Send up petri dishes containing bacteria Analyze the effects of temperature, pressure, and.
Brynn Larson Trey Karsten Terek Campbell Marcus Flores Marcell Smalley Shunsuke Miyazaki 2015/6/10 Team Ochocinco.
Transparent conducting oxides (TCOs) are often used in industrial applications. The utility of these semiconductors, as the name suggests, depends upon.
Excellence Justify the choice of your model by commenting on at least 3 points. Your comments could include the following: a)Relate the solution to the.
L 37 Modern Physics [3] [L37] Nuclear physics –what’s inside the nucleus and what holds it together –what is radioactivity –carbon dating [L38] Nuclear.
Radiation. When you see or hear this word what do you think about? What do you think it means? Share your thoughts with me by writing on the post it what.
Radiation. When you see or hear this word what do you think about? What do you think it means? Share your thoughts with me by writing on the post it what.
RESISTANCE. The resistance of a conductor is the ratio of the potential difference across it to the current flowing through it.
Slide # 1 Examples of pressure sensor packaging Temperature characteristics of a piezoresistive pressure sensor. Transfer function at three different temperatures.
Miscellaneous Notes: This is a bare-bones template – make it fancier if you wish, but be sure to address at least the items listed here. Basically this.
Vern J. Ostdiek Donald J. Bord Chapter 7 Electricity (Section 4)
Series-Parallel Combination Circuits
Lesson#23 Topic: Simple Circuits Objectives: (After this class I will be able to) 1. Explain the difference between wiring light bulbs in series and in.
The nucleus. Rutherford's nuclear atom (1902 ‑ 1920) Ernest Rutherford was interested in the distribution of electrons in atoms. Two of his students,
Seongbo Shim, Yoojong Lee, and Youngsoo Shin Lithographic Defect Aware Placement Using Compact Standard Cells Without Inter-Cell Margin.
FISICA AMBIENTALE 1 Radioattività: misure 1 Lezioni Marie Curie.
Lecture 16 Solving the Laplace equation in 2-D Remember Phils Problems and your notes = everything Only 6 lectures.
Radioactivity I §Content: §Radioactive substance §Three types of radiation §Properties of radiation §To investigate the radiation by apparatus §To summarize.
BOYLE’S LAW. WHAT IS BOYLE’S LAW? Boyle’s Law is one of the laws in physics that concern the behaviour of gases. At constant temperature it relates pressure.
STRUCTURES Outcome 3 Gary Plimer 2008 MUSSELBURGH GRAMMAR SCHOOL.
Mass Spectroscopy 1 Mass Spectroscopy (Mass Spec) Applying Atomic Structure Knowledge to Chemical Analysis.
Individual Subsystem Testing Report New Jersey Space Grant Consortium with Rutgers University Stevens Institute of Technology 2/13/2012.
Time series Model assessment. Tourist arrivals to NZ Period is quarterly.
RockSat-C 2012 SITR Full Mission Simulation Report University of Minnesota Alexander Richman Jacob Schultz Justine Topel Will Thorson 4/23/2012.
O Level Physics Chapter :24: Radiation and Half Life Prepared By: Shakil Raiman.
Thermionic Valves.
Ch 10.6: Other Heat Conduction Problems
Radioactivity By the end of this chapter you should be able to: describe the properties of alpha, beta and gamma radiations; explain why some nuclei are.
Mike Struik / LHC-CRI INSTRUMENTATION FEEDTHROUGH SYSTEM FOR LHC MACHINE ARC QUADRUPOLE MAGNETS. 123rd LHC Vacuum Design Meeting 19 April 1999.
Chapter V Radiation Detectors.
In many applications, a very pure form of a specific metal is required. One method used to purify a metal is called electrorefining. It uses a Type 3 Electrolytic.
DETECTION OF NUCLEAR RADIATION
Geiger-Mueller Counters Darwin L. Boyd Kent State University School of Technology.
PHYSICS – Radioactivity
8. Photo Electric Transducers:
Types Of Transducers Resistive Position Transducer: The principle of the resistive position transducer is that the physical variable under measurement.
ENERGY. Conservation of Energy: The total amount of energy in a system remains constant ("is conserved"), although energy within the system can be changed.
RPCs with Ar-CO2 mix G. Aielli; R.Cardarelli; A. Zerbini For the ATLAS ROMA2 group.
Sensors and Detectors - 2
Capacitance Chapter 26 (Continued) 1 30.
Geiger Tube Theory, Dead Time
Book 1 Section 5.1 The gas laws
Sensors and Detectors - 2
GCSE (1-9) Physics: Radioactivity Nuclear Decay and Half Life
Radiation Detectors : Detection actually means measurement of the radiation with its energy content and other related properties. The detection system.
TRIODE TUBES.
Atomic Physics & Quantum Effects
Scintillation Counter
Lise Johnson Phillip Forkner
STARTER WHAT QUESTIONS DO YOU WANT ANSWERED ABOUT NUCLEAR RADIATION?
Geiger-Mueller Tubes By: Daniel Hancock.
Radiation.
RADIATION AND HALF-LIFE
Radar Detection of Lightning
Presentation transcript:

Full Mission Simulation Test Report Cajun Probe University of Louisiana at Lafayette Mark Roberts

Mission Overview Objectives  Design and implement a robust, compact payload to latter be integrated into a probe.  Develop improved Geiger Counter circuit.  Testing of payload’s durability and performance under space conditions.  Obtain and analyze data for a baseline of future experiments.

Changes Since Subsystem Integration No changes have been made to the overall system so far Finished airtight chamber for pressure sensor and mount; The mount is made from a leftover polycarbonate makrolon sheet

Tests Performed (Thus far…) Geiger Plateau Geiger Plateau Pulse Height Pulse Height Dead Time Testing Dead Time Testing Overall Systems Function Test Overall Systems Function Test The Juicy source Life Test! The Juicy source Life Test! The Stay Puft Test! The Stay Puft Test! Snowman Test Snowman Test Deep South Test Deep South Test Appendix

Tests Results Defining the voltage range in which the Geiger-Mueller tube operates most effectively; that is, the region such that the potential difference in the tube is strong enough to ionize all the gas inside the tube upon triggering by the incoming ionizing radiation.

Voltages below the plateau are not high enough to cause complete discharge where as higher voltages causes quenching in which the positively charged ions are drawn to the cathode thus creating a continuous electric pulse in the counter.

Output Pulse An oscilloscope was used to measure the output electrical pulse of the avalanche at different operating voltages; the total charge of the pulse can be found by integrating the area under the contained in a pulse.

Pulse Height Pulse height generally increased fairly linearly as the increasing high voltage bias increased the electric field inside the Geiger Mueller detector thus allowing the discharge to grow larger.

Plotting the pulse height vs. operating voltage on a log-log scale further reveals a linear relationship suggesting a power law.

Dead Time (Gas Ionization Detectors) Dead Time: The minimum time between detectable pulses will be less than the recovery time. This is the pulse resolving time. Non-paralyzable dead-time: is defined as an event that occurs during this period is not counted nor does it influence the ability of the tube to respond to later events. Paralyzable dead time: is the time duration between the end of the non- paralyzable dead time and a resolving pint at which a pulse larger than the discriminator level can be developed.

Split Source Method to determine Dead Time A split radiation source is nothing more than a radioactive source that is split into two pieces. The source as a hole is considered to be the combined sources of N 1 and N 2 therefore I will call it N C. N 1 is the left side of the split source for me; making N 2 the right side of N C. Counts are taken from N 1, N 2, and N C sourced with the same time duration. Then the dead time of the system can be calculated by [seconds] I made my own split source with some Uranyl Acetate that was laying around which happens to contain Uranium 238! =o)

Dead Time of the Geiger Mueller tube with the Nuclear Scaler Model 500 The next series of tables are results from making specific adjustments to a particular section to the Geiger counter circuit in attempts to reduce dead time in the system…not all results are posted.

Will further investigate at a later time…

Overall Analysis Task to Complete For Launch Receive Geiger Counter PCB and construct counter Receive Geiger Counter PCB and construct counter Mounting of Geiger Tube(s) Mounting of Geiger Tube(s) Complete Assembly of payload Complete Assembly of payload Testing of complete Assembly Testing of complete Assembly Modification to standoffs Modification to standoffs

Lessons Learned Have at least one individual in charge of paperwork and producing the necessary documents. Have at least one individual in charge of paperwork and producing the necessary documents. Don’t play with high voltage with lack of sleep i.e. When applying high voltage to a breadboard the metal outer base of the breadboard is held at that potential consequently when your arm glances that part of the board…prepare for a wake up call… Don’t play with high voltage with lack of sleep i.e. When applying high voltage to a breadboard the metal outer base of the breadboard is held at that potential consequently when your arm glances that part of the board…prepare for a wake up call…

Appendix Test that were performed and included in last presentation Overall Systems Function Test Overall Systems Function Test The Juicy source life Test The Juicy source life Test The Stay Puft Test The Stay Puft Test The Snowman Test The Snowman Test The Deep South Test The Deep South Test

Overall Systems Function Test This test just involved hooking everything together and triggering each sensor to verify everything was behaving nominally. The Juicy source Life Test This just involved obtaining a hot radiation source (not the typical Cobalt 60 source), I settled on Cesium 137 and ran the counter for 16 hours. I don’t have any photos of this test bet lets just say the counter was going berserk the whole time. Video of counter with a Cobalt 60 source.

The Stay Puft Test The average off the shelf Marshmallow is a foam object with closed wall air cells within the foam. By placing a Marshmallow in a Vacuum the walls will expand with reduction of pressure; when air is allowed back into the chamber the walls collapse hence the marshmallow rapidly deflates to a shriveled state from it’s original form. By placing a Marshmallow in a Vacuum the walls will expand with reduction of pressure; when air is allowed back into the chamber the walls collapse hence the marshmallow rapidly deflates to a shriveled state from it’s original form. The Stay Puft Test is to demonstrate the effectiveness of the air tight containers' constructed. One marshmallow is placed inside the air tight container and then placed into the vacuum chamber along with another marshmallow.

Snowman Test The Snowman test is just a basic cold test where the payload is placed into a well insulated container and surrounded with dry ice to test the performance of the system(s) in a cold environment.

Deep South Test The Deep South test is designed to test the systems performance when heat is applied. Unfortunately all I had to my disposal was an industrial hot air gun. Thus to help distribute the hot air more evenly I threw together a black foam box (black body) and placed the payload inside this body with various temperature sensors placed through out it.

Deep South Test

Test Results: Stay Puft! Test Results: Snowman The marshmallow did indeed stay puft! Once tube reaches a particular temperature voltage drop off is dramatic

Test Results: Deep South Resulting effects….

Test Results: Deep South Temperature and Voltage are directly proportional here with a consequence of quenching occurring

Conclusions The results of the testing were as predicted however I did notice that the pressure sensor yields bogus data once it reaches a particular temperature in a cold environment. However, these temperatures will not be reached on the rocket but some type of insulation or a choice of another pressure sensor would solve this issue. Also from the snowman and deep south graphs if you notice the voltages ran. I was not able to use the LND tube due to a defection. It was replaced with an LND 712 tube. The only similarity between the two tubes are there temperature operational limits. I have already sent the defective LND tubes back to the manufacture for repair and will repeat these experiments again with the manufactured Geiger counter PCB and the LND tube.