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DeVry Phoenix - GF - trhyt
Complete exercises 9.3, 9.13, 9.15, 9.23, 9.42, 9.49.For problems requiring computations, please ensure that your Excel file includes the associated cellcomputations and/or statistics output
DeVry Phoenix - FVFD - vfdv
GuidetoNetworkDefenseandCountermeasures,2 ndEdition,ISBN:1418836796CHAPTER11&12,PAGE446&476IntrusionDetectionChapterQuiz11Name:_Date:_ChapterReviewQuestions,Strengthening&ManagingFirewalls1. Whichofthefollowingguidelinesshouldyoukeepinmindwhenedit
DeVry Phoenix - RTGED - ertfgre
Essay part 11. (TCO2)Organizationshavebothaninternalandanexternalenvironment.Describethegeneral environmentandgiveatleastonespecificexampleofeachdimension,otherthantheexamplesgivenin thetextandinthelectures.(Points : 20)2. (TCO3)Describethefourapproac
DeVry Phoenix - FRDE - rgrdfg
Legal Beagals Inc is a legal services firm that files incorporation papers for smallbusinesses. They charge $1,000 per application. This year's income statement shows thefollowing: Sales $1,440,000 Variable Expenses 1,008,000 Contribution margin 432,000
DeVry Phoenix - FRDEFG - vdfsv
1.In 2007 the Bureau of Justice Statistics released nationwide statistics on the prevalence of prison sexualviolence. Discuss the characteristics associated with perpetrators and victims of prison sexual violence. Whatare pervasive myths associated wit
DeVry Phoenix - DCSF - cdsc
Appendix HCOM/156 Version 51Associate Level MaterialAppendix ZOutline and Thesis Statement GuideType your approved or revised thesis statement below.Prepare a sentence outline for your paper, including references for points and/orsubpoints.This o
Indiana - PHYSICS - 301
Moseley : article sur les spectres des lments chimiques1 of 10http:/chimie.scola.ac-paris.fr/sitedechimie/hist_chi/text_origin/moseley/.THE HIGH FREQUENCY SPECTRA OF THE ELEMENTSBy H. G. J. Moseley, M. A.Phil. Mag. (1913), p. 1024In the absence of a
Indiana - PHYSICS - 301
Office Hours Next weekMonday 2:00 to 3:00Tuesday 1:00 to 3:30Wednesday 8:45 to 9:45Contact me if you need to meet at some timeother than that and we should be able toarrange something.P301 Final Exam ReviewThis file describes some of details of th
Indiana - PHYSICS - 301
Swain Hall West- 1 FloorStudentstServices office(drop/add)SecretarysofficeDVBsofficeSwain Hall West- 2 FloorndPhysics ForumAI office on thirdfloor 340LibraryLecturesCALM systemCALM system: First QuestionP301 Lecture 1 Welcome to P301;
Indiana - PHYSICS - 301
P301 Lecture 4Postulates of Special Relativity I- The laws of physics are the same in all inertialreference frames of reference (this is the same statementthat Galileo used) Note that the extra bits in the books statement are not quite correct.The l
Indiana - PHYSICS - 301
P301 Lecture 6Headlight effectThis effect is important in medium-energy physics experiments (lots of theaction is in the forward direction), and for synchrotron radiation sources(very bright sources of x-rays obtained from highly relativistic electron
Indiana - PHYSICS - 301
P301 Lecture 9X-RaysExperimental results on the absorption of xrays from C. G. Barkla Phil. Mag. 17 (1909)P301 Lecture 9X-Rayshttp:/www.google.com/imgres?imgurl=http:/www.amptek.comK and K lines from various elements(Mosely)http:/en.wikipedia.org/
Indiana - PHYSICS - 301
P301 Lecture 12Bohrs HypothesesBohr formulated the following ad hoc model:1.Atoms exist only in certain stable stationary states2.The dynamic equilibrium of these stationary states is determined bythe laws of classical physics, but the way the atoms
Indiana - PHYSICS - 301
P301 Lecture 17Matter Waves=h/pElectron diffraction using a Transmission Electron Microscopea). Single (quasi)-crystal (full sample is orientationally coherent)b). Polycrystalline material (many small crystals in all orientations).What is the wavele
Indiana - PHYSICS - 301
P301 Lecture 19Fourier Decomposition/analysishttp:/demonstrations.wolfram.com/WavepacketForAFreeParticle/http:/www.jhu.edu/signals/fourier2/index.htmlTwo-slit experiment withparticleshttp:/en.wikipedia.org/wiki/Double-slit_experimentSchrodingers Eq
Indiana - PHYSICS - 301
Schrodingers Equation SolutionsFinite Square WellFor this case, you must solve a transcendental equation to find the solutions thatobey the boundary conditions (in particular, continuity of the function and itsderivative at the well boundary). For the
Indiana - PHYSICS - 301
Lecture 25The Hydrogen Atom revisitedMajor differences between the QM hydrogenatom and Bohrs model (my list):The electrons do not travel in orbits, but in well defined states(orbitals) that have particular shapes (probability distributionsfor the el
Indiana - PHYSICS - 301
Lecture 27Hydrogen 3d, 4s and 4p3d4s4pWe can get some insight into the relativeEnergies of these three orbitals fromthe website:http:/keisan.casio.com/has10/SpecExec.cgihttp:/www.corrosionsource.com/handbook/periodic/periodic_table.gifLecture 27
Indiana - PHYSICS - 301
Lecture 31Exam II ResultsLecture 31Molecules and bondingWhy do atoms combine together to form molecules, and what forces/conceptscontrol the way this happens?How do molecules behave?http:/keisan.casio.com/has10/SpecExec.cgiLecture 31Molecules and
Indiana - PHYSICS - 301
BuildingamorecomplexmoleculeC2IsolatedimpuritiesFrom E. A. Moore: Molecular Modelling and bonding, Royal Soc. Chem.BuildingasolidGraphite/DiamondIsolatedimpuritiesFrom W. A. Harrison: Electron Structure Royal Soc. Chem.Buildingametal(Copper)Isolat
Indiana - PHYSICS - 301
SizeofNucleiT&R Figure 12.2R = ro A1/3ShellmodelforNucleiFrom E. SegreNuclei and Particles3-D HarmonicOscillatorSphericalSquare wellTrendsinNuclearStabilityT&R Figure 12.5See also Nudat2 at:http:/www.nndc.bnl.gov/nudat2/TrendsinNuclearStabi
Indiana - PHYSICS - 301
TypicalDecayschemeIINuclei can decrease theirproton number by one inthree ways, positronemission (the most common)Electron capture (muchmore rarely; see next slide),or proton emission (veryrare).Decay rates expressed interms of Becquerrel (1/sec
Indiana - PHYSICS - 301
Early categorization of ParticlesEarly collider experiments started to reveal more and more particles, andpeople started to question whether they were truly Fundamental, but didallow for the prediction of missing particles that were later found.Attemp
Indiana - PHYSICS - 301
beta=theta'cos(tht')010203040506070809010011012013014015016017017910.9848080.9396930.8660260.7660450.6427880.5000010.3420210.1736491.33E-006-0.173647-0.342019-0.499998-0.642786-0.766043-0.866024-0.939692-0.984807-0.
Indiana - PHYSICS - 301
I ) a) p=1V =-mtc';)l-C12 , trl <lreVJ'11V1J"'. 6"/'f e V (7 S I.f/ S"t! II Mqtr-=1-.1 ZJ WI / SCf . 5 't1)11"1- ?1JJf1&1/1)JL J ; :;-ur'/ff)' If -=-=-/,6rrxJi()eVJ:z.L ,'il( X / iYYJ5:.. I;? .J,rVIt\a. '" p r."r f (;f'1It1'1,t
Indiana - PHYSICS - 340
-l- C ~j:'t~1~'fJ7f!i .'\!.\To - /oDe-=i-IiJ . . .L (j'Jhiscfw_=-C-2iT q '-'- -I._-". " . - . " ~. ;:Ejx 19!/It(_,~'_?~? . ~?fJ2.. ':' L .lfcfw_ . /x.' ()'1-;r~._ . _. ,"_"._ .".".-.I_h)1. . , ,-~L . . .". . 1 . . . . . ... .
Indiana - PHYSICS - 340
P3'-t 0 1'1 w A :# 15P/IIl;f",f~oll.1"r8~ '~().'),~. j .'.'"'.~"~:_.~!:b;.<;/"'~ ~ ~ ~ ~j~.'~ ~.1~"Vh) -:.IF f/fJ I;:(t9f.~ ~z)P(~ -I~t) fJ + in.9'f (i)J J=IJ1CUJ,-=. .d<ert>/~P(2: f~ l) f .YII.!;~ gA .,~4 _ o.(f()"j.=(F~o~ill.
Indiana - PHYSICS - 340
P3LfO ,IfJ- ~s rf;t ~e"p-~;,._- - - - - -+- --0:-- - -._- -- --~-- -.- - .-. . tn1Di-i?/~. ~. ~ 6 ~-.-~-~-~~-iC~ _ GIlJ._ ._~-~2 _~.~ .~-~-~-1 ---'------.~1.It:e)i-[i.TrAJ- "pAlc.i?n ( -p 0(~ !I Al k [ 5/~h)Cp
Indiana - PHYSICS - 340
P 5'iJOF-ft;v 11 :If I L' Lq fr~:rr. ")' ' Ii '(3~ ./' , . ...J~ '. ... ~-?~... . .'!.-ol/~.~.~. . ~. .e.:r~ k(/\Tc1. . . .... f j ~ Tc:. .<.(r,>' . ~ 0 . ~ ~ ~ 8.:=.0 ~.~ . .r.~ 9. ." ~. ~ . rc ~. ~.-_-. ._._ ._ _. ._. _. . .K. eeL.=.'
Indiana - PHYSICS - 340
FvoYM.I i( 16(16.2),rivatives most oftenle o r pressure can be: following formulae,tie differentials o f t he5"-1,-.1'. fl(~ j ,'(,uT~~L aVlAavY L t 'FfA/t-t: volvm~ 5 '(fYi. ~. 5 i ( :5' r "d" I " 12 t :1L . /14 teO'- t' 'Y~a Y' I L,P.
Indiana - PHYSICS - 340
P3'-1 () ~;1rr X Lfb /u f-rJnf2 () 1/~ -~-'-~-~-'- -~'" - - -~--.-.-,-~-.-'-. -'"-.~-~- .-.---. - -=-_"_ _ _72,.c.~a3,C)_/.-~.-,-~-.- -.-~-~-~ ~_. _._ _ _ f_~_-.- - - -.-. -.-'--:.:P.- - - - -* --- .-_ ~Nlv-=-1;JV'-VI!~-!tN-vtf?
Indiana - PHYSICS - 340
LECTUREBaerleinSecionsTopics410-Jan12-Jan14-Jan17-Jan19-Jan1.1-1.41.5-1.72.1-2.2-2.3-2.5Introduction; Thermodynamic phenomenologyThe first two laws of thermodynamicsMicrostates and multiplicityMartin Luther King Day- NO CLASSElementary s
Indiana - PHYSICS - 340
Swain Hall West- 1st FloorStudentServices office(drop/add)SecretarysofficeDVBsofficeWeb site: http:/physics.indiana.edu/~courses/p340/S10/Swain Hall West- 2nd FloorPhysics ForumAI office on thirdfloor 340LibraryLecturesCALM systemNOTE: To
Indiana - PHYSICS - 340
P340 Lecture 3Probability and Statistics Bernoulli Trials REPEATED, IDENTICAL, INDEPENDENT, RANDOMtrials for which there are two outcomes (successprob.=p; failure prob=q) EXAMPLES: Coin tosses, queuing problems, radioactivedecay, scattering experim
Indiana - PHYSICS - 340
P340 Lecture 5(Second Law)THE FUNDAMENTAL POSTULATE(OF THERMAL PHYSICS) Any isolated system in thermodynamic equilibrium is equallylikely to be in any one of its available microstatesTHE SECOND LAW OF THERMODYNAMICS Any isolated thermodynamic syste
Indiana - PHYSICS - 340
Lecture 8 Carnot Cycle SH = -|QH|/TH SC = |QC|/TC S = SH + SC =0=> |QH|/TH = |QC|/TChttp:/thermodynamicstudy.net/carnot.htmlThe most efficient heat engine would be one that does not change theentropy of the universe (i.e. the decrease of the sour
Indiana - PHYSICS - 340
Lecture 12- CALMThe so-called two-level system is a model that finds many uses in physics. Inthis model, the system is assumed to have only two states in which it can exist,and these states are separated in energy by an amount . Consider asituation in
Indiana - PHYSICS - 340
Lecture 15- CALMWhat would you most like me to discuss tomorrow in preparation for theupcoming exam? proton)? Partition Function/Canonical Ensemble (3) Efficiency/Engine Cycles (3) Examples (3) Taylor expansions, looking at limits (2) Adiabatic pro
Indiana - PHYSICS - 340
P301 Lecture 8CMB fit to BB spectrumThe plot on the right shows data from theFIRAS instrument on the original COBEsatellite experiment. The measurement ofinterest here was the set of residuals (i.e.the lower plot of the differences between themeasu
Indiana - PHYSICS - 340
P301 Lecture 8CMB fit to BB spectrumThe plot on the right shows data from theFIRAS instrument on the original COBEsatellite experiment. The measurement ofinterest here was the set of residuals (i.e.the lower plot of the differences between themeasu
Indiana - PHYSICS - 340
Lecture 21 Examples Chpt. 7Lecture 21 Examples Chpt. 7Langmuir AdsorptionqP=[kBT/l3] [q/(1-q)] exp(-eo/kBT)http:/en.wikipedia.org/wiki/Langmuir_adsorption_modelCryopumpsWhy do they pump N2 more effectively than He?He is smaller/lighter etc. (5 ans
Indiana - PHYSICS - 340
Lecture 21 Examples Chpt. 7Lecture 21 Examples Chpt. 7Langmuir AdsorptionP=[kBT/3] [/(1-)] exp(o/kBT)http:/en.wikipedia.org/wiki/Langmuir_adsorption_modelCryopumpsWhy do they pump N2 more effectively than He?He is smaller/lighter etc. (5 answers)B
Indiana - PHYSICS - 340
Spin-statistics theoremAs we discussed in P301, all sub-atomic particles with which we haveexperience have an internal degree of freedom known as intrinsic spin, whichcomes in integral multiples of hbar/2 (i.e. h/4p, so it has dimensions ofangular mom
Indiana - PHYSICS - 340
Spin-statistics theoremAs we discussed in P301, all sub-atomic particles with which we haveexperience have an internal degree of freedom known as intrinsic spin, whichcomes in integral multiples of hbar/2 (i.e. h/4, so it has dimensions ofangular mome
Indiana - PHYSICS - 340
Laser Cooling/Trapping of atomshttp:/www.ptb.de/en/org/4/44/443/melcol_e.jpgWe will discuss this in more detail toward the end of the semester, but it ispossible to slow-down (cool) atoms by passing them through a region withcounter-oriented laser bea
Indiana - PHYSICS - 340
Laser Cooling/Trapping of atomshttp:/www.ptb.de/en/org/4/44/443/melcol_e.jpgWe will discuss this in more detail toward the end of the semester, but it ispossible to slow-down (cool) atoms by passing them through a region withcounter-oriented laser bea
Indiana - PHYSICS - 340
Examples: ReifShow that CP and CV may be related to each other through quantities that may bedetermined from the equation of state (i.e. by knowing V as a function of P, T, and N)Note, what Reif labels a, is what we have already introduced as bP.Examp
Indiana - PHYSICS - 340
Examples: ReifShow that CP and CV may be related to each other through quantities that may bedetermined from the equation of state (i.e. by knowing V as a function of P, T, and N)Note, what Reif labels , is what we have already introduced as P.Example
Indiana - PHYSICS - 340
Heat Capacity of diatomic gasesNote: thetemperature scale ishypotheticalhttp:/www.phys.unsw.edu.au/COURSES/FIRST_YEAR/pdf%20files/x.%20Equipartion.pdfExample 11.9 from BaierleinA gas of the HBr is in thermal equilibrium. At what temperature will the
Indiana - PHYSICS - 340
Exam II ResultsAvg.Exam Results33.8=56%4.543.5Students32.52Frequency1.510.502025303540Grade45505560Exam questions1. A typical neutron star has a radius of 12 km and a density of roughly 5x10 17 kg/m3 (which is only slightly great