HomeWork Simulations of Particle Interactions with Matter
Homework 1
1.) Maxwell Boltzmann
Given the Maxwell -Boltzmann Distribution
a.) Show <v>
Show that
b.) Energy Fluctuation (Grad)
Show that the energy fluctuation is
- Note
- = velocity fluctuation
2.) MC calculation of Pi
Calculate Notes
using the Monte Carlo method described in the
You may use the program I gave you in the lab for this but you must change the program to indicate that you were able to understand its structure and you were able to recompile it.
Cheater go here: http://physics.isu.edu/~tforest/Classes/NucSim/Day1/PI_MC/
3.) Histograms using ROOT
Create histograms of the random numbers stored in the ROOT ntuple created in in Problem 2 above.
try
rns->Draw("rnd1*4"); rns->Draw("rnd1:rnd1","rnd1>0.5"); rns->Draw("asin(rnd1)"); rns->Draw("asin(rnd1-rnd2)"); Does this look like a Normal/Gaussian Distributi on?
Homework 2
1.) Derive Rutherford Formula
Derive the Rutherford Scattering formula.
2.) EXN02 in GEANT
You will learn how to setup your Unix environment to compile EXN02 from the GEANT4 distribution
a.) Compile and run the default version of ExN02 in GEANT4
You can use a computer screen shot to prove you did this.
b.) Now make your own copy of it and change the target material
Homework 3
Write a "How TO" document describing how to download and install the latest version of
Use a screen shot to prove you did it.
Suggested answers to a few questions asked when running "./Configure -build"
Hints:
- First step, install the version of CLHEP recommended on the GEANT4 website.
- Second step, build without graphics and static libraries
Do you want to build 'shared' (.so) libraries? [n] n G4UI_NONE Do you want to set this variable ? [n] y G4VIS_NONE If this variable is set, no visualization drivers will be built or used. Do you want to set this variable ? [n] y
- Third step, now turn on the visualization
Do you want to build 'shared' (.so) libraries? [n] n G4UI_NONE If this variable is set, no UI sessions nor any UI libraries are built. This can be useful when running a pure batch job or in a user framework having its own UI system. Do you want to set this variable ? [n] G4UI_BUILD_XAW_SESSION G4UI_USE_XAW Specifies to include and use the XAW interfaces in the application to be built. The XAW (X11 Athena Widget set) extensions are required to activate and build this driver. [y] G4UI_BUILD_XM_SESSION G4UI_USE_XM Specifies to include and use the XM Motif based user interfaces. The XM Motif extensions are required to activate and build this driver. [y] G4VIS_BUILD_OPENGLX_DRIVER G4VIS_USE_OPENGLX It is an interface to the de facto standard 3D graphics library, OpenGL. It is well suited for real-time fast visualization and prototyping. The X11 version of the OpenGL libraries is required. [y] G4VIS_BUILD_OPENGLXM_DRIVER G4VIS_USE_OPENGLXM It is an interface to the de facto standard 3D graphics library, OpenGL. It is well suited for real-time fast visualization and prototyping. The X11 version of the OpenGL libraries and the Motif Xm extension is required. [y] OGLHOME/include OGLHOME/lib You have selected to use OpenGL driver. Specify the correct path (OGLHOME) where OpenGL is installed in your system. It was found in: [/usr]
An old version of Installation notes
Visualization Libraries:
Homework 4
1.) Use GEANT4 to simulate the calculation the energy loss of a charged particle through LH2. In class I showed an example for an incident 10 MeV proton. You need to pick another particle (pion, kaon, muon ...) and a different energy. Compare your answer with the Triumf curveFile:SPIM HydrogenStoppingPower.pdf.
2.) Compute
for the heavy charged particle you chose to simulate in problem 1. Use the particle's energy at one of the tracking steps and compare to what GEANT4 found.Homework 5
1.) Show that the maximum energy transfered to thin absorbers for a relativistic head on collision is
- = momentum of incident heavy charged ion of mass
- = mass of target electron initially at rest
2.) Use GEANT4 to determine the Range of the particle chosen in Homework 4 through liquid hydrogen as a function of Energy.
Homework 6
1.) You need to lower the beam energy of 600 MeV protons to 400 MeV using a slab of copper. The density of the copper is 8.962
. Determine how thick the copper should be by integrating the stopping power curve:Stopping Power of several particles through Copper as a function of energy is shown in this curve. File:StoppingPowerInCopper.pdf
2.) Alter GEANT4 example N02 to check your answer for problem 1 above. I expect you to hand in a screen shot showing GEANT4 tracking the proton from 600 MeV to 400 MeV.
3.) Find
using GEANT4 for a 600 MeV proton traveling through a slab of copper. You will need to make the copper thick enough to stop the proton. Then output the stopping distance to a file which you can read into ROOT using some of the software we used for Homework 1's RNG problem.Homework 7
Media:SPIM_BremE-Spectrum-Tantalum.pdf
Media:SPIM_LaTex_TemplateFile.txt
Homework 8
Homework 9
1.) Write a Paragraph (4 - 5 sentences) desribing the Simulation you would like to perform as your Project for this class. You will need to write a title. You will need to specify the reaction you will be simulating.
Use the Latex skeleton file below to format your document
Media:SPIM_LaTex1_TemplateFile.txt
some commands:
latex filename dvips filename -o temp.ps pdflatex filename
Homework 10
Homework 11
There are 2 parts to this homework. First you will compare relative rates for the PhotoElectric, Compton, and pair production physics processes using the same target you used in Homework 10. Second you will write another section of your project which describes the experimental results you are going to compare to using GEANT4.
1.) Compare Photoelectric, Compton and pair production rates relative to eachother using the same target used in the last Homework assignment (#10).
a.) first turn on all three physics processes for a gamma particle in the physics list.
b.) add variables to the output which can be used to identify which physics process is responsible for the event being written to the output file.
c.) Run the simulation so the incident photon energy spans energies from 100 eV to 10 GeV.
d.) Use ROOT to plot a 3-D representation of the Process type on one axis, the incident photon energy on the other axis and the number of counts along the z-axis.
A bad example of such a plot for a 30 cm long Argon gas target is given in the file
Yours will have better labels
Hint:
->Draw("ProcesID:Egamma","","lego");
2.) Add another section to your project report which describes the experimental measurements you will be using to compare to GEANT4. I am expecting to see a plot and references.
Homework 12
The objective of this homework is to compare the number of collisions needed to thermalize a neutron in GEANT to the expected number of collisions using the Neutron Slowing Down Theory described in class.
1.) Add neutron physics process to your physics list
#include "G4LElastic.hh" #include "G4NeutronHPElastic.hh" #include "G4NeutronHPorLElastic.hh"
} else if (particleName == "neutron") { //neutron // available neutron elastic scattering models // G4LElastic* elasticModel = new G4LElastic(); //G4NeutronHPElastic* elasticModel = new G4NeutronHPElastic(); G4NeutronHPorLElastic* elasticModel = new G4NeutronHPorLElastic(); // define process to handle elastic scattering G4HadronElasticProcess* hadElastProc = new G4HadronElasticProcess(); // register the model you are using for eleastic scattering hadElastProc->RegisterMe(elasticModel); // add the elastic scattering process to the process manager pmanager->AddDiscreteProcess(hadElastProc); // label LElastic in tracker
}
Use a Liquid Hydrogen target
G4Material* LH2 = new G4Material("Hydrogen", z=1., a= 1.01*g/mole, density= 0.07*g/cm3, kStateGas,3*kelvin,1.7e5*pascal);
change the target to be a 60 cm square and 60 cm thick in Z (a 60 cm cube)
fTargetLength = 60 * cm; // Full length of Target
solidTarget = new G4Box("target",fTargetLength,fTargetLength,targetSize);
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