A second order system
|
|
- Estella Whitehead
- 6 years ago
- Views:
Transcription
1 The Link Between The Phase Magin And The Convete Tansient Response Chistophe BASSO ON Seionduto 4, ue Paul Mesplé BP TOULOUSE Cedex - Fane When designing a losed-loop syste, a swith-ode powe supply fo instane, a path is eated between the vaiable you want to onito and the ontol pin of you onvete. This ontol pin an be the peak uent set point in a uent-ode powe supply o the duty-yle input with a voltage-ode ontolle. If the onitoed vaiable deviates fo its iposed taget, the ontolle eats by eithe ineasing o deeasing the deliveed powe to the load via an aplified eo signal fed to its ontol pin. The powe stage, howeve, is affeted by a gain and a phase that ae fequeny dependent, H(s). To ake sue the esulting powe supply will behave pe the speified data, it is the designe task to shape the etun path G(s) to opensate fo the powe stage esponse at etain fequeny points. Aong the ipotant paaetes ae the d gain fo the sallest stati eo and the lowest output ipedane, but also the oss ove fequeny fo the equied esponse speed. At the oss ove point, whee the loop gain odule T(s) equals, the etuning signal will be affeted by a etain phase otation. If the signal etuns in phase with the ontol signal, we have onditions to fo an osillato, soething you want to avoid. To ake sue the signal does not etun in phase, that is to say with a 36 phase otation, you ust plan a etain aount of agin between the phase otation of T(s) at the oss ove fequeny and the 36 liit: this is the phase agin. Howeve, how uh phase agin should you ask to obine pefoane and stable answe? 45 as often found in the books, oe than that? Let us disove how uh though the following lines. A seond ode syste Figue shows a LC low-pass filte whee the esisto R illustates the losses in the netwok. This ahitetue ould be seen as a siplified lossy output filte of an unloaded buk onvete. In that ase, the input voltage V in epesents the aveage level of the squae wave signal pesent at the powe swith/feewheel diode athode juntion. Fo the pupose of this study, this aveage voltage will be a odulated and we ae looking fo the expession of the output voltage aoss the output apaito. We will then alulate the tansfe funtion H(s) = V out (s)/v in (s) of this stutue. 3 R {R} L {L} Vout Vin C {C} paaetes f=35k L=u C=/(4*3.459^*f^*L) w=({l}*{c})^-.5 Q= R=/((({C}/(4*{L}))^.5)**{Q}) Figue : a buk onvete an be epesented by a siple low-pass filte. The sipt at the botto autoates the alulation of R when hanging the Q value. Using Laplae notation, () desibes the tansfe funtion H(s) of this RLC netwok: = H s LCs + RCs + () By e-aanging the expession, it beoes possible to identify the quality oeffiient Q and the esonant fequeny.
2 s s s s + ζ Q = = H s () Whee, is the esonant fequeny, ζ (zeta) is the daping fato and Q, the quality oeffiient: C = (3), ζ = R (4), Q LC 4L = ζ (5) The idea is now to evaluate the esponse to a -V input step and hange the quality oeffiient values by tweaking the esisto R. This esisto is epesentative of the losses in the netwok suh as the Equivalent Seies Resisto of the induto fo instane. As you an ead in Figue, we have autoated the alulation of R whose value is evaluated aoding to the seleted Q. We ould also ultiply () by /s and alulate the invese Laplae tansfo to obtain the tepoal esponse. A SPICE siulation will be faste in ou ase. The esults appea in Figue. Plot vout#6, vout#5, vout#4, vout#3, vo ut in volts Q = 5 Q = Q =.77 Q =.5 Q <.5 ove daping Q =.5 itial daping Q >.5 unde daping Oveshoot = 65% Asyptotially stable Fast esponse and no oveshoot! 789 Q =. 5.u 5.u 5.u 35.u 45.u tie in seonds Figue : when Q is swept fo. to 5, the answe to a step is eithe slow (Q =.) but without oveshoot o faste, with a lage oveshoot fo big Q values. As one an see, low Q values lead to a opletely osillation fee esponse wheeas values above.5 give bith to oveshoots. As Q ineases, eaning less losses, the oveshoot gets lage. If Q would go to infinity, it would iply an undaped LC netwok keeping osillations going futhe to an exitation. Looking fo oots The study of () denoinato will eveal the oots fo whih H(s) goes to infinity. Matheatially, it oesponds to the following haateisti equation: s s + + = (6) Q Whee the oots oe easily as follows: ( Q ) s, s = ± 4 (7) Q
3 In (7), the te unde the squae oot an eithe be positive o negative, depending on the quality oeffiient value. Fo Q values below.5, the so-alled ovedaped ase, the te unde the squae oot eains positive and both oots s and s ae sepaated eal oots. The step esponse is sluggish as shown in Figue. When Q eahes.5, alled the itially daped ase, the oots ae still eal but ae now oinident. The step esponse is uh faste but still does not exhibit oveshoot. Now, if Q futhe gows, we ae in an undedaped ase and the oots weloe an iaginay potion that ineases as Q goes up: we have a fast step esponse now featuing oveshoot and osillations. If Q eahes infinity, the eal potion of oots s and s fades away and the syste feely osillates: thee is no oe daping (losses) bought by the eal tes. Analysing the tajetoy of these oots is alled oot lous analysis: it shows how the oots ae positioned in the s-plane and give indiation on how they ove in elationship to soe paaetes. It is Q in this exaple but it ould be the gain k of a syste whee, at soe point when k is ineased, the oots igate in the ight half plane and eate an instability. Figue 3 desibes the path taken by s and s as Q hanges. j Q = High Q Low Q Low Q σ Q =.5 High Q LHP RHP Figue 3: oot lous analysis helps to undestand how the oots ove in elationship to a seleted paaete, hee the quality oeffiient of ou LC netwok. Appoxiation of an open-loop esponse Based on what we have aleady dislosed, it would be inteesting to odel ou losed-loop d-d onvete with an equation whee a quality oeffiient te would appea. That way, we ould selet the paaete that affets this Q to shape the output esponse we ae looking fo: slow but without any oveshoot o, on the opposite, faste but aepting a little oveshoot. Let us stat the deivation poess by looking at Figue 4: 8 8. T(s) Phase ( ) Module (db) db f agt( s ) agt(f ) 5 ϕ k k k fequeny in hetz Figue 4: the open-loop esponse of a opensated buk onvete an be appoxiated to a seond-ode syste in the viinity of the oss ove fequeny. This figue shows the oplete loop gain T(s) ade of the onvete powe stage tansfe funtion H(s) futhe shaped by the opensato tansfe funtion, G(s). This exaple is dealing with a CCM buk onvete opeated
4 in voltage-ode ontol. In this figue, we onentate on the aea aound the oss ove fequeny f whih epesents one ipotant design paaete of the d-d onvete you ty to stabilize. Asyptotially looking at the uve within the fae eveals the effets of an oigin pole and a high fequeny pole. Matheatially, this appoxiation an be foulated by: s s + (8) In this appoxiated expession, we onside exta poles and zeos fa away fo f, natually liiting thei ipat on the tansfe funtion. Howeve, ou inteest lies in the esponse the d-d onvete is going to delive one its loop is losed. In othe tes, let us identify the losed-loop tansfe funtion deived fo (8). To + : obtain the losed expession, we an evaluate + = s s + + (9) Equation (9) appeas aanged in fo that ealls that of (). Theefoe, we an put it unde the failia fo of a seond ode syste as desibed by (): + = s s + + Q () The identifiation of the quality oeffiient Q and the esonant fequeny is staightfowad: and = (). Q = () We now have an equation that desibes the appoxiated losed-loop esponse of ou d-d and it inludes a quality oeffiient. The next step is to establish a elationship between the losed-loop Q and the key design paaete, the open-loop phase agin. Fist, based on (8), let us alulate the oss ove fequeny bought by the loation of the oigin pole and its assoiated high fequeny pole. At the oss ove point, we know that the T(s) odule equals. Theefoe: j j + = (3) Extating and e-aanging gives:
5 + 4 = (4) If we substitute ( ()) into (4), we obtain a Q-dependent oss ove fequeny : 4 ( + Q ) 4 = (5) Equation (5) shows us how the losed-loop quality oeffiient and the open-loop oss ove fequeny ae linked. It is ipotant fo this eak to be well undestood: Q epesents the esulting losed-loop esponse quality oeffiient based on the open-loop pole/zeo aangeent desibing the appoxiated open-loop opensated tansfe funtion T(s) in (8). To ontinue futhe with ou analysis, we evaluate the phase otation of T(s) at the oss ove fequeny: agt ( ) = tan + tan = tan (6) The phase agin ϕ epesents the distane between the total phase otation at the oss ove fequeny given by (6) and the 8 liit. In this ase, we puposely neglet the phase evesal bought by the opeational aplifie. Hene, we have: ϕ = + agt (7) Substituting (6) into (7), we obtain: ϕ = tan = tan (8) Reebeing ou fa fa away tigonoeti lasses (!), we have: tan x + tan = (9) x Thanks to (9), we an update ()(6): ϕ = tan () We have aleady defined the oss ove fequeny vesus the losed loop quality oeffiient in (5). If we apitalize on this definition in (), we have:
6 ϕ = tan ( Q ) () The next step is to extat the losed-loop quality oeffiient fo () and siplify the esult: ( ϕ) ( ϕ ) ( ϕ) ( ϕ ) 4 + tan os Q = = () tan sin This is it! We now have a elationship between ou ain design iteion the open-loop phase agin and the quality oeffiient ou loop will exhibit one losed. The best is to exploe the vaious Q diffeent phase agin hoies will bing though a gaph as poposed by Figue Q + tan( φ) 4 5 ϕ tan ( φ ) φ Figue 5: the gaph shows the evolution of the losed-loop quality oeffiient as you selet diffeent phase agin. If you want to obine speed and lak of oveshoot, Figue suggests a Q of.5. Reading the oesponding phase agin in Figue 5, we an see a design iteion of 76 satisfies this equest fo suh a Q, fa away fo the 45 found in the ajoity of text books! What does it ean then? In the esponse to a load step, one the loop is losed, the open-loop phase agin ostly affets the eovey shape and a little the undeshoot depth. Theefoe, it eally depends on the kind of esponse you ae looking fo o what the ustoe speifiations ipose on you design. If a fast eovey is needed and a little oveshoot aepted, then eduing the phase agin an be an option. On the ontay, if absolutely no oveshoots ae toleated, you have no hoie than ineasing the phase agin to the detient of the eovey speed. Whateve solution you selet, you have to ake sue that whateve the opeating onditions, input/output, tepeatue and noal paaeti vaiations (ESRs fo instane), the phase agin neve goes below 45. In othe wods, shooting fo a typial value aound 7 should beoe a good design patie. Tansient esponse and phase agin We have stabilized the buk onvete using one of the autoated siulation platfos desibed in Ref. []. The tehnique allows to keep the sae oss ove fequeny while playing on the phase agin only. The oveall shape is the sae as that pesented in Figue 4 with a -khz oss ove fequeny. The output is subjeted to step anging fo A to A in µs. The esults appea in Figue 6. The 76 phase agin gives a little oveshoot of.5% wheeas the 49 agin tiples that oveshoot, still easonable though given the vetial axis sale of V pe division. Howeve, you an obseve a faste eovey in the 49 phase ase (7 µs) vesus the 76 ase (7 µs). Why do we still have oveshoot with the 76 when theoy states thee should be none? It is beause (8) is a siplified view of the tansfe funtion in the viinity of the oss ove fequeny. As detailed in Ref. [], if you have thee o oe poles installed nea the oss ove fequeny, the Q fato
7 appoxiation we have been though does not wok anyoe and exta wok is equied. Nevetheless, as exeplified by Figue 6, a sall phase agin leads to a peaky losed-loop esponse ϕ = 36 ϕ = ϕ = 64 V out (t) V/div 4.96 ϕ = t 5 µs/div 8u Figue 6: the phase agin has been adjusted at diffeent values and it lealy affets the tansient esponse in both the eovey tie and the oveshoot above the 5-V taget. Conlusion The design of a powe onvete equies aes when it oes to loop ontol. Nueous text books just eoend to design fo a 45 phase agin without any explanations. This atile shows how to analytially deive a phase agin taget whih is supisingly highe than 45 and lose to 76. Despite soe appoxiations at the beginning of the study, the final esult is baked up by siulation esults that onfi the need fo a phase agin geate than the lassial 45 eoendations. Refeenes. C. Basso, Swith Mode Powe Supplies: SPICE Siulations and Patial Designs, MGaw-Hill, 8. R. Eikson, D. Maksiovi, Fundaentals of Powe Eletoni, Kluwes Aadei Pess,
Suppose you have a bank account that earns interest at rate r, and you have made an initial deposit of X 0
IOECONOMIC MODEL OF A FISHERY (ontinued) Dynami Maximum Eonomi Yield In ou deivation of maximum eonomi yield (MEY) we examined a system at equilibium and ou analysis made no distintion between pofits in
More informationDetermine the Stress Calculating Mode of Sliding Failure of Soil Mass under the Push-Extend Multi-under-Reamed Pile
Engineeing, 014, 6, 54-59 Published Online Apil 014 in SiRes. http://www.sip.og/jounal/eng http://dx.doi.og/10.436/eng.014.6509 Deteine the Stess Calulating Mode of Sliding Failue of Soil Mass unde the
More informationChapter 4. Sampling of Continuous-Time Signals
Chapte 4 Sampling of Continuous-Time Signals 1 Intodution Disete-time signals most ommonly ou as epesentations of sampled ontinuous-time signals. Unde easonable onstaints, a ontinuous-time signal an be
More informationExtra Examples for Chapter 1
Exta Examples fo Chapte 1 Example 1: Conenti ylinde visomete is a devie used to measue the visosity of liquids. A liquid of unknown visosity is filling the small gap between two onenti ylindes, one is
More informationRed Shift and Blue Shift: A realistic approach
Red Shift and Blue Shift: A ealisti appoah Benhad Rothenstein Politehnia Uniesity of Timisoaa, Physis Dept., Timisoaa, Romania E-mail: benhad_othenstein@yahoo.om Coina Nafonita Politehnia Uniesity of Timisoaa,
More informationExperiment 1 Electric field and electric potential
Expeiment 1 Eleti field and eleti potential Pupose Map eleti equipotential lines and eleti field lines fo two-dimensional hage onfiguations. Equipment Thee sheets of ondutive papes with ondutive-ink eletodes,
More informationGeneralized Vapor Pressure Prediction Consistent with Cubic Equations of State
Genealized Vapo Pessue Pedition Consistent with Cubi Equations of State Laua L. Petasky and Mihael J. Misovih, Hope College, Holland, MI Intodution Equations of state may be used to alulate pue omponent
More informationATMO 551a Fall 08. Diffusion
Diffusion Diffusion is a net tanspot of olecules o enegy o oentu o fo a egion of highe concentation to one of lowe concentation by ando olecula) otion. We will look at diffusion in gases. Mean fee path
More informationNumerical Modeling in Biomedical Systems
Numeial Modeling in Biomedial Systems BME 15:35 Letue 7 9/6/17 Nonlinea Systems Dunn Chapte 5 Nonlinea equations Root finding Baketing methods Open methods Gaphial Bisetion False Position Newton s method
More informationBasic Bridge Circuits
AN7 Datafoth Copoation Page of 6 DID YOU KNOW? Samuel Hunte Chistie (784-865) was bon in London the son of James Chistie, who founded Chistie's Fine At Auctionees. Samuel studied mathematics at Tinity
More informationPhysics 218, Spring March 2004
Today in Physis 8: eleti dipole adiation II The fa field Veto potential fo an osillating eleti dipole Radiated fields and intensity fo an osillating eleti dipole Total satteing oss setion of a dieleti
More information30 The Electric Field Due to a Continuous Distribution of Charge on a Line
hapte 0 The Electic Field Due to a ontinuous Distibution of hage on a Line 0 The Electic Field Due to a ontinuous Distibution of hage on a Line Evey integal ust include a diffeential (such as d, dt, dq,
More informationME 3600 Control Systems Frequency Domain Analysis
ME 3600 Contol Systems Fequency Domain Analysis The fequency esponse of a system is defined as the steady-state esponse of the system to a sinusoidal (hamonic) input. Fo linea systems, the esulting steady-state
More informationSAMPLE LABORATORY SESSION FOR JAVA MODULE B. Calculations for Sample Cross-Section 2
SAMPLE LABORATORY SESSION FOR JAVA MODULE B Calulations fo Sample Coss-Setion. Use Input. Setion Popeties The popeties of Sample Coss-Setion ae shown in Figue and ae summaized below. Figue : Popeties of
More informationRecitation PHYS 131. must be one-half of T 2
Reitation PHYS 131 Ch. 5: FOC 1, 3, 7, 10, 15. Pobles 4, 17, 3, 5, 36, 47 & 59. Ch 5: FOC Questions 1, 3, 7, 10 & 15. 1. () The eloity of a has a onstant agnitude (speed) and dietion. Sine its eloity is
More informationLecture 23: Central Force Motion
Lectue 3: Cental Foce Motion Many of the foces we encounte in natue act between two paticles along the line connecting the Gavity, electicity, and the stong nuclea foce ae exaples These types of foces
More informationCorrespondence Analysis & Related Methods
Coespondene Analysis & Related Methods Oveview of CA and basi geometi onepts espondents, all eades of a etain newspape, osstabulated aoding to thei eduation goup and level of eading of the newspape Mihael
More informationFARADAY'S LAW. dates : No. of lectures allocated. Actual No. of lectures 3 9/5/09-14 /5/09
FARADAY'S LAW No. of lectues allocated Actual No. of lectues dates : 3 9/5/09-14 /5/09 31.1 Faaday's Law of Induction In the pevious chapte we leaned that electic cuent poduces agnetic field. Afte this
More informationChapter 2: Basic Physics and Math Supplements
Chapte 2: Basic Physics and Math Supplements Decembe 1, 215 1 Supplement 2.1: Centipetal Acceleation This supplement expands on a topic addessed on page 19 of the textbook. Ou task hee is to calculate
More informationTidal forces. m r. m 1 m 2. x r 2. r 1
Tidal foces Befoe we look at fee waves on the eath, let s fist exaine one class of otion that is diectly foced: astonoic tides. Hee we will biefly conside soe of the tidal geneating foces fo -body systes.
More informationNon-Ideal Gas Behavior P.V.T Relationships for Liquid and Solid:
hemodynamis Non-Ideal Gas Behavio.. Relationships fo Liquid and Solid: An equation of state may be solved fo any one of the thee quantities, o as a funtion of the othe two. If is onsideed a funtion of
More information3.6 Applied Optimization
.6 Applied Optimization Section.6 Notes Page In this section we will be looking at wod poblems whee it asks us to maimize o minimize something. Fo all the poblems in this section you will be taking the
More informationLECTURE 15. Phase-amplitude variables. Non-linear transverse motion
LETURE 5 Non-linea tansvese otion Phase-aplitude vaiables Second ode (quadupole-diven) linea esonances Thid-ode (sextupole-diven) non-linea esonances // USPAS Lectue 5 Phase-aplitude vaiables Although
More informationmatschek (ccm2548) Ch17-h3 chiu (57890) 1
matshek m2548) Ch17-h3 hiu 5789) 1 This pint-out should have 16 questions. Multiple-hoie questions may ontinue on the next olumn o page find all hoies efoe answeing. 1 1. points A student said, The eleti
More informationOrbital Angular Momentum Eigenfunctions
Obital Angula Moentu Eigenfunctions Michael Fowle 1/11/08 Intoduction In the last lectue we established that the opeatos J Jz have a coon set of eigenkets j J j = j( j+ 1 ) j Jz j = j whee j ae integes
More information1 Fundamental Solutions to the Wave Equation
1 Fundamental Solutions to the Wave Equation Physial insight in the sound geneation mehanism an be gained by onsideing simple analytial solutions to the wave equation One example is to onside aousti adiation
More informationFrom E.G. Haug Escape Velocity To the Golden Ratio at the Black Hole. Branko Zivlak, Novi Sad, May 2018
Fom E.G. Haug Esape eloity To the Golden Ratio at the Blak Hole Banko Zivlak, bzivlak@gmail.om Novi Sad, May 018 Abstat Esape veloity fom the E.G. Haug has been heked. It is ompaed with obital veloity
More informationAVS fiziks. Institute for NET/JRF, GATE, IIT-JAM, JEST, TIFR and GRE in PHYSICAL SCIENCES
ELECTROMAGNETIC THEORY SOLUTIONS GATE- Q. An insulating sphee of adius a aies a hage density a os ; a. The leading ode tem fo the eleti field at a distane d, fa away fom the hage distibution, is popotional
More informationPhotographing a time interval
Potogaping a time inteval Benad Rotenstein and Ioan Damian Politennia Univesity of imisoaa Depatment of Pysis imisoaa Romania benad_otenstein@yaoo.om ijdamian@yaoo.om Abstat A metod of measuing time intevals
More informationDissolution of Solid Particles in Liquids: A Shrinking Core Model
Wold Aademy of Siene, Engineeing and Tehnology 5 9 Dissolution of Solid Patiles in Liquids: A Shining oe Model Wei-Lun Hsu, Mon-Jyh Lin, and Jyh-Ping Hsu Astat The dissolution of spheial patiles in liquids
More informationOSCILLATIONS AND GRAVITATION
1. SIMPLE HARMONIC MOTION Simple hamonic motion is any motion that is equivalent to a single component of unifom cicula motion. In this situation the velocity is always geatest in the middle of the motion,
More informationFARADAY'S LAW dt
FAADAY'S LAW 31.1 Faaday's Law of Induction In the peious chapte we leaned that electic cuent poduces agnetic field. Afte this ipotant discoey, scientists wondeed: if electic cuent poduces agnetic field,
More informationdp p v= = ON SHOCK WAVES AT LARGE DISTANCES FROM THE PLACE OF THEIR ORIGIN By Lev D. Landau J. Phys. U.S.S.R. 9, 496 (1945).
ON SHOCK WAVES AT LARGE DISTANCES FROM THE PLACE OF THEIR ORIGIN By Lev D. Landau J. Phys. U.S.S.R. 9, 496 (1945). It is shown that at lage distanes fom the body, moving with a. veloity exeeding that of
More informationEddy Currents and Magnetic Calibrations in LDX using a Copper Plasma. D.P. Boyle, PPPL M.E. Mauel, D.T. Garnier, Columbia J.
Eddy Cuents and Magneti Calibations in LDX using a Coppe Plasma D.P. Boyle PPPL M.E. Mauel D.T. Ganie Columbia J. Kesne MIT PSFC Coppe Plasma Oveview LDX Magnetis Goals Calibate magneti diagnostis positions
More informationAnswers to Coursebook questions Chapter 2.11
Answes to Couseook questions Chapte 11 1 he net foe on the satellite is F = G Mm and this plays the ole of the entipetal foe on the satellite, ie mv mv Equating the two gives π Fo iula motion we have that
More information8-3 Magnetic Materials
11/28/24 section 8_3 Magnetic Mateials blank 1/2 8-3 Magnetic Mateials Reading Assignent: pp. 244-26 Recall in dielectics, electic dipoles wee ceated when and E-field was applied. Q: Theefoe, we defined
More informationCOMPARING MORE THAN TWO POPULATION MEANS: AN ANALYSIS OF VARIANCE
COMPARING MORE THAN TWO POPULATION MEANS: AN ANALYSIS OF VARIANCE To see how the piniple behind the analysis of vaiane method woks, let us onside the following simple expeiment. The means ( 1 and ) of
More informationPHYS 110B - HW #7 Fall 2005, Solutions by David Pace Equations referenced as Eq. # are from Griffiths Problem statements are paraphrased
PHYS B - HW #7 Fall 5, Solutions by David Pae Equations efeened as Eq. # ae fom Giffiths Poblem statements ae paaphased [.] Poblem.4 fom Giffiths Show that Eq..4, V, t an be witten as Eq..44, V, t q t
More informationOBSTACLE DETECTION USING RING BEAM SYSTEM
OBSTACLE DETECTION USING RING BEAM SYSTEM M. Hiaki, K. Takamasu and S. Ozono Depatment of Peision Engineeing, The Univesity of Tokyo 7-3-1 Hongo, Bunkyo-ku, Tokyo, Japan Abstat: In this pape, we popose
More information2.5 The Quarter-Wave Transformer
/3/5 _5 The Quate Wave Tansfome /.5 The Quate-Wave Tansfome Reading Assignment: pp. 73-76 By now you ve noticed that a quate-wave length of tansmission line ( λ 4, β π ) appeas often in micowave engineeing
More informationRelated Rates - the Basics
Related Rates - the Basics In this section we exploe the way we can use deivatives to find the velocity at which things ae changing ove time. Up to now we have been finding the deivative to compae the
More informationPhysics 2B Chapter 22 Notes - Magnetic Field Spring 2018
Physics B Chapte Notes - Magnetic Field Sping 018 Magnetic Field fom a Long Staight Cuent-Caying Wie In Chapte 11 we looked at Isaac Newton s Law of Gavitation, which established that a gavitational field
More information1 Fundamental Solutions to the Wave Equation
1 Fundamental Solutions to the Wave Equation Physial insight in the sound geneation mehanism an be gained by onsideing simple analytial solutions to the wave equation. One example is to onside aousti adiation
More informationLab 10: Newton s Second Law in Rotation
Lab 10: Newton s Second Law in Rotation We can descibe the motion of objects that otate (i.e. spin on an axis, like a popelle o a doo) using the same definitions, adapted fo otational motion, that we have
More informationReview for the previous lecture
Review fo the pevious letue Definition: sample spae, event, opeations (union, intesetion, omplementay), disjoint, paiwise disjoint Theoem: ommutatitivity, assoiativity, distibution law, DeMogan s law Pobability
More informationMolecular Energy Changes During a Reaction
Reation Kinetis Moleula Enegy Changes Duing a Reation Chemial Enegy of Speies E xn E* +BP E* P+B Moleules above this enegy level (defined somewhat abitaily) ae alled ativated omplexes Poduts Reatants Pogession
More informationThe geometric construction of Ewald sphere and Bragg condition:
The geometic constuction of Ewald sphee and Bagg condition: The constuction of Ewald sphee must be done such that the Bagg condition is satisfied. This can be done as follows: i) Daw a wave vecto k in
More informationSPH4U Unit 6.3 Gravitational Potential Energy Page 1 of 9
SPH4 nit 6.3 Gavitational Potential negy Page of Notes Physics ool box he gavitational potential enegy of a syste of two (spheical) asses is diectly popotional to the poduct of thei asses, and invesely
More informationCHAPTER 5: Circular Motion; Gravitation
CHAPER 5: Cicula Motion; Gavitation Solution Guide to WebAssign Pobles 5.1 [1] (a) Find the centipetal acceleation fo Eq. 5-1.. a R v ( 1.5 s) 1.10 1.4 s (b) he net hoizontal foce is causing the centipetal
More informationSimulation of a Shielded Thermocouple
ISSN 1014-4874 DOI : http://dx.doi.og/10.4314/j.v27i1.1 Siulation of a Shielded Theoouple Fedik Bentsson 1, Fidèle Ndahayo, Yves Nyalihaa and, Jean Maie Vianney Munyeshyaka 2 1 Linköping Univesity, S-581
More informationAddendum to Nonperturbative QED: Muon Structure and Decay
Applied Physis Reseah; Vol. 6, No. 6; 04 ISSN 96-9639 E-ISSN 96-9647 Published by Canadian Cente of Siene and Eduation Addendu to Nonpetubative QED: Muon Stutue and Deay Buke Rithie Lawene Liveoe National
More informationExperiment I Voltage Variation and Control
ELE303 Electicity Netwoks Expeiment I oltage aiation and ontol Objective To demonstate that the voltage diffeence between the sending end of a tansmission line and the load o eceiving end depends mainly
More informationAlgebra-based Physics II
lgebabased Physics II Chapte 19 Electic potential enegy & The Electic potential Why enegy is stoed in an electic field? How to descibe an field fom enegetic point of view? Class Website: Natual way of
More informationAdsorption and Desorption Kinetics for Diffusion Controlled Systems with a Strongly Concentration Dependent Diffusivity
The Open-Access Jounal fo the Basic Pinciples of Diffusion Theoy, Expeient and Application Adsoption and Desoption Kinetics fo Diffusion Contolled Systes with a Stongly Concentation Dependent Diffusivity
More informationSo, if we are finding the amount of work done over a non-conservative vector field F r, we do that long ur r b ur =
3.4 Geen s Theoem Geoge Geen: self-taught English scientist, 793-84 So, if we ae finding the amount of wok done ove a non-consevative vecto field F, we do that long u b u 3. method Wok = F d F( () t )
More informationExploration of the three-person duel
Exploation of the thee-peson duel Andy Paish 15 August 2006 1 The duel Pictue a duel: two shootes facing one anothe, taking tuns fiing at one anothe, each with a fixed pobability of hitting his opponent.
More informationAPPENDIX D COMPRESSIBILITY FACTOR EQUATIONS D.1 THE REDLICH KWONG EQUATION
AENDIX D COMRESSIBILIY FACOR EQUAIONS D.1 HE REDLICH KWONG EQUAION he Redlih-Kwong equation is atually an equation of state. It was fomulated by Otto Redlih and Joseph N. S. Kwong in 1949 [Chemial Review
More informationSchool of Electrical and Computer Engineering, Cornell University. ECE 303: Electromagnetic Fields and Waves. Fall 2007
School of Electical and Compute Engineeing, Conell Univesity ECE 303: Electomagnetic Fields and Waves Fall 007 Homewok 8 Due on Oct. 19, 007 by 5:00 PM Reading Assignments: i) Review the lectue notes.
More informationPhysics 161 Fall 2011 Extra Credit 2 Investigating Black Holes - Solutions The Following is Worth 50 Points!!!
Physics 161 Fall 011 Exta Cedit Investigating Black Holes - olutions The Following is Woth 50 Points!!! This exta cedit assignment will investigate vaious popeties of black holes that we didn t have time
More informationCircular Orbits. and g =
using analyse planetay and satellite motion modelled as unifom cicula motion in a univesal gavitation field, a = v = 4π and g = T GM1 GM and F = 1M SATELLITES IN OBIT A satellite is any object that is
More informationr ˆr F = Section 2: Newton s Law of Gravitation m 2 m 1 Consider two masses and, separated by distance Gravitational force on due to is
Section : Newton s Law of Gavitation In 1686 Isaac Newton published his Univesal Law of Gavitation. This explained avity as a foce of attaction between all atte in the Univese, causin e.. apples to fall
More informationKepler s problem gravitational attraction
Kele s oblem gavitational attaction Summay of fomulas deived fo two-body motion Let the two masses be m and m. The total mass is M = m + m, the educed mass is µ = m m /(m + m ). The gavitational otential
More information(a) Calculate the apparent weight of the student in the first part of the journey while accelerating downwards at 2.35 m s 2.
Chapte answes Heineann Physics 1 4e Section.1 Woked exaple: Ty youself.1.1 CALCULATING APPARENT WEIGHT A 79.0 kg student ides a lift down fo the top floo of an office block to the gound. Duing the jouney
More informationSAMPLE QUIZ 3 - PHYSICS For a right triangle: sin θ = a c, cos θ = b c, tan θ = a b,
SAMPLE QUIZ 3 - PHYSICS 1301.1 his is a closed book, closed notes quiz. Calculatos ae pemitted. he ONLY fomulas that may be used ae those given below. Define all symbols and justify all mathematical expessions
More informationA New I 1 -Based Hyperelastic Model for Rubber Elastic Materials
A New I -Based Hypeelastic Model fo Rubbe Elastic Mateials Osca Lopez-Paies SES Octobe -4, Evanston, IL Neo-Hookean odel W ìï ï ( I - ) = ( if l + l + l - ) lll = = í ï + othewise ïî (*). Matheatical siplicity
More informationTo Feel a Force Chapter 7 Static equilibrium - torque and friction
To eel a oce Chapte 7 Chapte 7: Static fiction, toque and static equilibium A. Review of foce vectos Between the eath and a small mass, gavitational foces of equal magnitude and opposite diection act on
More informationClass 6 - Circular Motion and Gravitation
Class 6 - Cicula Motion and Gavitation pdf vesion [http://www.ic.sunysb.edu/class/phy141d/phy131pdfs/phy131class6.pdf] Fequency and peiod Fequency (evolutions pe second) [ o ] Peiod (tie fo one evolution)
More information(Sample 3) Exam 1 - Physics Patel SPRING 1998 FORM CODE - A (solution key at end of exam)
(Sample 3) Exam 1 - Physics 202 - Patel SPRING 1998 FORM CODE - A (solution key at end of exam) Be sue to fill in you student numbe and FORM lette (A, B, C) on you answe sheet. If you foget to include
More information6 PROBABILITY GENERATING FUNCTIONS
6 PROBABILITY GENERATING FUNCTIONS Cetain deivations pesented in this couse have been somewhat heavy on algeba. Fo example, detemining the expectation of the Binomial distibution (page 5.1 tuned out to
More informationSolution to HW 3, Ma 1a Fall 2016
Solution to HW 3, Ma a Fall 206 Section 2. Execise 2: Let C be a subset of the eal numbes consisting of those eal numbes x having the popety that evey digit in the decimal expansion of x is, 3, 5, o 7.
More informationPhysics 2A Chapter 10 - Moment of Inertia Fall 2018
Physics Chapte 0 - oment of netia Fall 08 The moment of inetia of a otating object is a measue of its otational inetia in the same way that the mass of an object is a measue of its inetia fo linea motion.
More informationThe Kerr-metric, mass- and light-horizons, and black holes' radii.
006 Thiey De Mees The Ke-meti, mass- and light-hoizons, and blak holes' adii. (using the Analogue Maxwell theoy) T. De Mees - thieydm @ pandoa.be Abstat Blak holes an geneally be defined as stella objets
More informationClassical Approach to the Theory of Elementary Particles
Classial Appoah to the Theoy of Elementay Patiles By Yui N. Keilman Abstat: Pesented hee is an attempt to modify /extend lassial eletodynamis (CED) in ode to enable the lassial appoah (the appoah based
More informationMotithang Higher Secondary School Thimphu Thromde Mid Term Examination 2016 Subject: Mathematics Full Marks: 100
Motithang Highe Seconday School Thimphu Thomde Mid Tem Examination 016 Subject: Mathematics Full Maks: 100 Class: IX Witing Time: 3 Hous Read the following instuctions caefully In this pape, thee ae thee
More informationMathematisch-Naturwissenschaftliche Fakultät I Humboldt-Universität zu Berlin Institut für Physik Physikalisches Grundpraktikum.
Mathematisch-Natuwissenschaftliche Fakultät I Humboldt-Univesität zu Belin Institut fü Physik Physikalisches Gundpaktikum Vesuchspotokoll Polaisation duch Reflexion (O11) duchgefüht am 10.11.2009 mit Vesuchspatne
More informationReflectance spectra for Si
Refletane speta fo Si Notie R and ε i and ε show onsideable stutues in the fom of peas and shouldes. These stutues aise fom the optial tansitions between alene bands to the ondution bands. 16 Miosopi Theoy:
More informationOptimum Settings of Process Mean, Economic Order Quantity, and Commission Fee
Jounal of Applied Science and Engineeing, Vol. 15, No. 4, pp. 343 352 (2012 343 Optiu Settings of Pocess Mean, Econoic Ode Quantity, and Coission Fee Chung-Ho Chen 1 *, Chao-Yu Chou 2 and Wei-Chen Lee
More information(n 1)n(n + 1)(n + 2) + 1 = (n 1)(n + 2)n(n + 1) + 1 = ( (n 2 + n 1) 1 )( (n 2 + n 1) + 1 ) + 1 = (n 2 + n 1) 2.
Paabola Volume 5, Issue (017) Solutions 151 1540 Q151 Take any fou consecutive whole numbes, multiply them togethe and add 1. Make a conjectue and pove it! The esulting numbe can, fo instance, be expessed
More informationInvestigation of Magnitude and Phase Errors in Waveguide Samples for the Nicolson-Ross-Weir Permittivity Technique
Univesity of New Hampshie Univesity of New Hampshie Sholas' Repositoy Maste's Theses and Capstones Student Sholaship Winte 016 Investigation of Magnitude and Phase Eos in Waveguide Samples fo the Niolson-Ross-Wei
More informationMacro Theory B. The Permanent Income Hypothesis
Maco Theoy B The Pemanent Income Hypothesis Ofe Setty The Eitan Beglas School of Economics - Tel Aviv Univesity May 15, 2015 1 1 Motivation 1.1 An econometic check We want to build an empiical model with
More informationASTR415: Problem Set #6
ASTR45: Poblem Set #6 Cuan D. Muhlbege Univesity of Mayland (Dated: May 7, 27) Using existing implementations of the leapfog and Runge-Kutta methods fo solving coupled odinay diffeential equations, seveal
More information4) Magnetic confinement of plasma
4) Magneti onfineent of plasa Due to the shielding in the plasa, thee is alost no ontol with eleti fields. A ontol is possible with agneti fields, as patiles ae bound to the field lines. This is alled
More informationMath 2263 Solutions for Spring 2003 Final Exam
Math 6 Solutions fo Sping Final Exam ) A staightfowad appoach to finding the tangent plane to a suface at a point ( x, y, z ) would be to expess the cuve as an explicit function z = f ( x, y ), calculate
More informationNatural Convection Heat Transfer Effects with Micro Finned Structures
Natual Convetion Heat Tansfe Effets with Mio Finned Stutues Saad MAHMOUD, Raya AL-DADAH*, David ASPINWALL, Leung SOO * Coesponding autho: Tel.: ++44(0)114143513; Fax: ++44(0)114143958; Email:.k.aldadah@bham.a.uk
More informationCHAPTER 3. Section 1. Modeling Population Growth
CHAPTER 3 Section 1. Modeling Population Gowth 1.1. The equation of the Malthusian model is Pt) = Ce t. Apply the initial condition P) = 1. Then 1 = Ce,oC = 1. Next apply the condition P1) = 3. Then 3
More informationGame Study of the Closed-loop Supply Chain with Random Yield and Random Demand
, pp.105-110 http://dx.doi.og/10.14257/astl.2014.53.24 Gae Study of the Closed-loop Supply Chain with ando Yield and ando Deand Xiuping Han, Dongyan Chen, Dehui Chen, Ling Hou School of anageent, Habin
More informationHandout: IS/LM Model
Econ 32 - IS/L odel Notes Handout: IS/L odel IS Cuve Deivation Figue 4-4 in the textbook explains one deivation of the IS cuve. This deivation uses the Induced Savings Function fom Chapte 3. Hee, I descibe
More informationCapacitors and Capacitance
Capacitos and Capacitance Capacitos ae devices that can stoe a chage Q at some voltage V. The geate the capacitance, the moe chage that can be stoed. The equation fo capacitance, C, is vey simple: C Q
More informationLC transfer of energy between the driving source and the circuit will be a maximum.
The Q of oscillatos efeences: L.. Fotney Pinciples of Electonics: Analog and Digital, Hacout Bace Jovanovich 987, Chapte (AC Cicuits) H. J. Pain The Physics of Vibations and Waves, 5 th edition, Wiley
More informationLecture 8 - Gauss s Law
Lectue 8 - Gauss s Law A Puzzle... Example Calculate the potential enegy, pe ion, fo an infinite 1D ionic cystal with sepaation a; that is, a ow of equally spaced chages of magnitude e and altenating sign.
More informationBetween any two masses, there exists a mutual attractive force.
YEAR 12 PHYSICS: GRAVITATION PAST EXAM QUESTIONS Name: QUESTION 1 (1995 EXAM) (a) State Newton s Univesal Law of Gavitation in wods Between any two masses, thee exists a mutual attactive foce. This foce
More informationAnisotropic 2-D Wavelet Packets and Rectangular Tiling: Theory and Algorithms
Anisotopi -D Wavelet Pakets and Retangula Tiling: Theoy and Algoithms Dan Xu and Minh N. Do Depatment of Eletial and Compute Engineeing and Bekman Institute Univesity of Illinois at Ubana-Champaign Email:
More informationNuclear and Particle Physics - Lecture 20 The shell model
1 Intoduction Nuclea and Paticle Physics - Lectue 0 The shell model It is appaent that the semi-empiical mass fomula does a good job of descibing tends but not the non-smooth behaviou of the binding enegy.
More informationRESONANCE SERIES RESONANT CIRCUITS. 5/2007 Enzo Paterno 1
ESONANCE SEIES ESONANT CICUITS 5/007 Enzo Pateno ESONANT CICUITS A vey impotant cicuit, used in a wide vaiety o electical and electonic systems today (i.e. adio & television tunes), is called the esonant
More informationThe Research of AQI Index Changing Regularity Mainly in Tianjin Ziyu Guo
nd Intenational Confeene on Eduation Tehnology, Management and Humanities Siene (ETMHS 06 The Reseah of AQI Index Changing Regulaity Mainly in Tianjin Ziyu Guo Shool of Institute of Eletial and Eletoni
More informationarxiv: v4 [physics.class-ph] 14 Jul 2018
Noname manusipt No. will be inseted by the edito Long-Range Longitudinal Eleti Wave in Vauum Radiated by Eleti Dipole: Pat I Altay Zhakatayev, Leila Tlebaldiyeva axiv:7.v4 [physis.lass-ph] 4 Jul 8 Reeived:
More information2. Equation of generalized Dynamics. Let rectangular right hand coordinate triple is fixed in three-dimensional Euclidian space.
Genealized Dynamis about Foes Ating on Chage Moving in Capaito and Solenoid. J.G. Klyushin, Ph. D. Aademy of Civil Aviation, hai of applied mathematis; e-mail: klyushin@shaping.og; mail: Intenational Club
More informationChapter 6 Differential Analysis of Fluid Flow
1 Chapte 6 Diffeential Analysis of Fluid Flow Inviscid flow: Eule s equations of otion Flow fields in which the sheaing stesses ae zeo ae said to be inviscid, nonviscous, o fictionless. fo fluids in which
More information7.2.1 Basic relations for Torsion of Circular Members
Section 7. 7. osion In this section, the geomety to be consideed is that of a long slende cicula ba and the load is one which twists the ba. Such poblems ae impotant in the analysis of twisting components,
More informationGain-Scheduled Controller Design: An Analytic Framework Directly Incorporating Non-Equilibrium Plant Dynamics
Gain-Sheduled Contolle Design: An Analyti Fameok Dietly Inopoating Non-Equilibium Plant Dynamis D.J.Leith W.E.Leithead Abstat Depatment of Eletoni & Eletial Engineeing, Univesity of Stathlyde, GLASGOW
More information