Physics Courseware Modern Physics
|
|
|
- Annabella Richard
- 6 years ago
- Views:
Transcription
1 Physis Cousewae oden Physis Enegy and oentu Relatiisti oentu: p γ Kineti enegy: K. E. ( γ ) Auxiliay equation: E + 4 p whee is the est ass and E is total enegy. Poble.- What has oe ass at est: i) A sodiu 3 Na nuleus ii) potons and neutons Solution: The nuleus has less ass. The diffeene in ass ties is the binding enegy. Poble.- Calulate the total enegy of a uon (whose ass at est is 06eV/ ) that is oing at a speed of Solution: Enegy γ γ (0.97) So, Enegy γ 4.345(06eV/ ) 436 ev Poble 3.- If the kineti enegy of a patile of ass is equal to its est enegy, how uh is its oentu? (A) p (B) p (C) p 3 (D) p (E) p 0. 5 Solution: we use the anillay equation: ( + ) p + 4 p 4 E p p p 3 answe: C
2 Poble 3a.- What is the speed of a poton whose kineti enegy is thee ties its est enegy? Solution: Aoding to the poble K.E.3, so: K.E. ( γ ) 3 ( γ ) γ 4 But γ, so: / 4 / / 6 / / Poble 3b.- If the kineti enegy of a patile of ass is equal to fou ties its est enegy, then the agnitude of the patile s elatiisti oentu is: Solution: Aoding to the poble K.E. 4, so the total enegy is E 5 and using the anillay equation: E p + ( 5 ) p + 5 p + Soling fo p: 4 p 4 p 4 Poble 3.- If the kineti enegy of a patile of ass is equal to twie its est enegy, then the agnitude of the patile s elatiisti oentu is: Solution: Aoding to the poble K.E., so the total enegy is E 3 and using the anillay equation: E p + ( 3 ) p + 9 p + Soling fo p: 4 p 8 p 8 Poble 4.- How uh enegy do you need to gie an eleton to aeleate it fo est to 0.99? Gie you answe in eleton olts. (A) 3.eV (B) 4.eV (C) 5.eV (D) 6.eV (E) 7.eV
3 Solution: we alulate the kineti enegy: K.E. (γ ) eV ( ) ev answe: A Poble 5.- A lup of lay whose est ass is 4 gas is taeling at 3/5 the speed of light when it ollides head-on with an idential lup going the opposite dietion at the sae speed. If the two lups stik togethe and no enegy is adiated away, what is the ass of the oposite lup? (A) 4g (B) 6.4g (C) 8g (D) 0g (E) 3.3g Solution: we alulate the total enegy befoe and afte: 4g TEbefoe TEafte γ γ 0g ( 3/ 5) 0.6 answe: D Poble 6.- A patile leaing a yloton has a total elatiisti enegy of 0 and a elatiisti oentu of 8 /. What is the est ass of this patile? (A) 0.5 (D) 6 (B). (E) 6 (C) Solution: we use the anillay equation: E p + ( 0 ) (8/) answe: D Poble 6a.- A patile leaing a yloton has a total elatiisti enegy of.3 ev and a elatiisti oentu of. ev/. What is the est ass of this patile? Poble 6: Using the anillay equation: 4 4 E p + (.3eV ) (.ev / ) + Soling fo : eV.44eV + ev
4 Poble 7.- Deonstate that if the foe is paallel to the eloity of a patile you an wite Newton s seond law of otion as 3 F γ a dp Solution: Aoding to Newton s seond law: F whih is still alid in speial dt elatiity, but we need to use the elatiisti oentu, not p as in lassial physis. If the foe and eloity ae paallel we an dop the eto notation and teat the poble as a one diensional poble: dp dγγ d d d F dt dt dt / d / dt Notie that we used the hain ule of deiaties and also notie that d/dt is the aeleation a, so the foe beoes: / / d / / + / F a a a d 3/ / / ( / ) a 3 γ a 3/ ( / ) Note: Be aeful when using this foula that is the eloity of the patile, not the eloity of a fae of efeene. Reebe that this is only alid if the foe and eloity ae paallel. Poble 8.- A patile of ass deays fo est into two patiles. One patile has ass and the othe patile is assless. The oentu of the assless patile is: ( ( A) 4 ( ( B) ( ( C) ) ) ) ( ) ( D) 4( ( E) )
5 Solution: Conseation of enegy: 4 + p + p p + p p p answe (B) Poble 9.- What is the kineti enegy of an eleton whose speed is K. E. γ Solution: ( ) 79? 37 In joules: 4 K. E J, and in ev: K. E. 5keV
4) 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
Recitation 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
r dt dt Momentum (specifically Linear Momentum) defined r r so r r note: momentum is a vector p x , p y = mv x = mv y , p z = mv z
Moentu, Ipulse and Collisions Moentu eeyday connotations? physical eaning the tue easue of otion (what changes in esponse to applied foces) d d ΣF ( ) dt dt Moentu (specifically Linea Moentu) defined p
Lecture 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
GRAVITOELECTROMAGNETISM AND NEWTON S LAW OF UNIVERSAL GRAVITATION
GAVITOELECTOMAGNETIM AND NEWTON LAW O UNIVEAL GAVITATION Antoine Ake etied Pofesso, Depatent Industial ienes Uniesity Collee Kaho int-lieen Gent - Beliu ant.ake@skynet.be Abstat In this atile it is shown
GRAVITOELECTROMAGNETISM AND NEWTON S LAW OF UNIVERSAL GRAVITATION
GAVITOELECTOMAGNETIM AND NEWTON LAW O UNIVEAL GAVITATION Antoine Ake etied Pofesso, Depatent Industial ienes Uniesity Collee Kaho int-lieen Gent - Beliu ant.ake@skynet.be Abstat Takin into aount the kineatis
VISUAL PHYSICS ONLINE EQUATION MINDMAPS
VISUAL PHYSICS ONLIN QUATION MINDMAPS quation ae eential pat of phyi, without them, we an t tat to explain ou phyial wold and make pedition. An equation tell a toy a olletion of a few ymbol ontain a wealth
EN40: Dynamics and Vibrations. Midterm Examination Tuesday March
EN4: Dynaics and Vibations Midte Exaination Tuesday Mach 8 16 School of Engineeing Bown Univesity NME: Geneal Instuctions No collaboation of any kind is peitted on this exaination. You ay bing double sided
Equivalency of Momentum and Kinetic Energy and Pythagorean Conservation of Mass and Energy
Intenational Jounal of Applied Physis and Matheatis, Vol., No. 4, July quivaleny of Moentu and Kineti negy and Pythagoean Consevation of Mass and negy Mohsen Lutey Abstat Aepted equations in the ehanis
In electrostatics, the electric field E and its sources (charges) are related by Gauss s law: Surface
Ampee s law n eletostatis, the eleti field E and its soues (hages) ae elated by Gauss s law: EdA i 4πQenl Sufae Why useful? When symmety applies, E an be easily omputed Similaly, in magnetism the magneti
Circular Motion Problem Solving
iula Motion Poblem Soling Aeleation o a hange in eloity i aued by a net foe: Newton nd Law An objet aeleate when eithe the magnitude o the dietion of the eloity hange We aw in the lat unit that an objet
System of Particles: Center-of-Mass
System of Paticles: Cente-of-ass The cente-of-mass of a system of paticles is the point that moes as though () all of the systems mass wee concentated thee and () all etenal foces wee applied thee. Location
Chapter 28 Special Relativity
Galilean Relatiity Chapter 8 Speial Relatiity A passenger in an airplane throws a ball straight up. It appears to oe in a ertial path. The law of graity and equations of otion under unifor aeleration are
Doppler Effect (Text 1.3)
Doppler Effet (et 1.3) Consider a light soure as a soure sending out a tik eery 1/ν and these tiks are traeling forward with speed. tik tik tik tik Doppler Effet (et 1.3) Case 1. Obserer oing transersely.
(Newton s 2 nd Law for linear motion)
PHYSICS 3 Final Exaination ( Deeber Tie liit 3 hours Answer all 6 questions You and an assistant are holding the (opposite ends of a long plank when oops! the butterfingered assistant drops his end If
1121 T Question 1
1121 T1 2008 Question 1 ( aks) You ae cycling, on a long staight path, at a constant speed of 6.0.s 1. Anothe cyclist passes you, tavelling on the sae path in the sae diection as you, at a constant speed
Physics 43 HW 2 Chapter 39 Problems given from 7 th Edition
Physis 3 HW Chater 39 Problems gien from 7 th Edition Problems:, 7,, 9, 1, 0,,, 9, 33, 35, 3, 0, 5,. How fast must a meter stik be moing if its length is measured to shrink to 0.500 m? P39. L = L L Taking
LINEAR MOMENTUM Physical quantities that we have been using to characterize the motion of a particle
LINEAR MOMENTUM Physical quantities that we have been using to chaacteize the otion of a paticle v Mass Velocity v Kinetic enegy v F Mechanical enegy + U Linea oentu of a paticle (1) is a vecto! Siple
Gravitational Equivalent Frequency, the Planck Length and Matter Waves
Gaitational Equialent Fequeny, te Plank Lengt and Matte Waes by Roge Ellman Abstat Analysis of gaitation and of matte waes disloses a geate signifiane tan eetofoe eognized fo te fequeny, wae, osillation
FARADAY'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,
ATMO 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
SPH4U 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
4. Compare the electric force holding the electron in orbit ( r = 0.53
Electostatics WS Electic Foce an Fiel. Calculate the magnitue of the foce between two 3.60-µ C point chages 9.3 cm apat.. How many electons make up a chage of 30.0 µ C? 3. Two chage ust paticles exet a
Tolga Yarman. Okan University, Akfirat, Istanbul and Savronik, Sanayii Merkezi, Eskiehir, Turkey.
Intenational Jounal of the Physial Sienes ol. 5(7, pp. 679-74, 8 Deebe, Aailable online at http://www.aadeijounals.og/ijps ISSN 99-95 Aadei Jounals Full Length Reseah Pape Wae-like inteation, ouing at
1131 T Question 1
1131 T1 2008 Question 1 ( aks) You ae cycling, on a long staight path, at a constant speed of 6.0.s 1. Anothe cyclist passes you, taelling on the sae path in the sae diection as you, at a constant speed
Charged particle motion in magnetic field
Chaged paticle otion in agnetic field Paticle otion in cued agnetic fieldlines We diide the equation of otion into a elocity coponent along the agnetic field and pependicula to the agnetic field. Suppose
For circular motion with tangential acceleration we get:
FW Phys 13 E:\Exel files\h1-18 Fomulas eiew fo final4.do page 1 of 1 Last pinted 5/19/4 :4: PM Kinemati fomulas: x = a = onstant (1.1) = α = onstant Pojetile Motion: 1 The inemati equation eto t () = at
Example 1. Centripetal Acceleration. Example 1 - Step 2 (Sum of Vector Components) Example 1 Step 1 (Free Body Diagram) Example
014-11-18 Centipetal Aeleation 13 Exaple with full olution Exaple 1 A 1500 kg a i oing on a flat oad and negotiate a ue whoe adiu i 35. If the oeffiient of tati fition between the tie and the oad i 0.5,
Red 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,
The Planck Mass Particle Finally Discovered! The True God Particle! Good bye to the Point Particle Hypothesis!
The Plank Mass Patile Finally Disoveed! The Tue God Patile! Good bye to the Point Patile Hypothesis! Espen Gaade Haug Nowegian Univesity of Life Sienes Septembe, 06 Abstat In this pape we suggest that
CHAPTER 6: UNIFORM CIRCULAR MOTION AND GRAVITATION
College Physics Student s Manual Chapte 6 CHAPTER 6: UIORM CIRCULAR MOTIO AD GRAVITATIO 6. ROTATIO AGLE AD AGULAR VELOCITY. Sei- taile tucks hae an odoete on one hub of a taile wheel. The hub is weighted
Ch. 4: FOC 9, 13, 16, 18. Problems 20, 24, 38, 48, 77, 83 & 115;
WEEK-3 Recitation PHYS 3 eb 4, 09 Ch. 4: OC 9, 3,, 8. Pobles 0, 4, 38, 48, 77, 83 & 5; Ch. 4: OC Questions 9, 3,, 8. 9. (e) Newton s law of gavitation gives the answe diectl. ccoding to this law the weight
Today: Review of SR. Einstein s Postulates of Relativity (Abbreviated versions) Let's start with a few important concepts
Today: eiew of Eam: Tomorrow, 7:30-9:00pm, DUANE GB30 You an bring paper (etter format written on both sides with whateer you think might help you during the eam. But you annot bring the tetbook or leture
momentum change via particle gain/
Letue 6 asi plasa dynais Ou fluid euations that we developed befoe ae: f ( n n )+ v v n + v v M v f P+ n E+ v 3 4 34 oentu lost via ollisions oentu hange via patile gain/ loss We have looked ollisions
matschek (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
If the speed of light were smaller than it is, would relativistic phenomena be more or less conspicuous than they are now?
Physis 07 Problem. If the speed of light were smaller than it is, would relatiisti phenomena be more or less onspiuous than they are now? All of the phenomena of speial relatiity depend upon the fator
Chapter Outline The Relativity of Time and Time Dilation The Relativistic Addition of Velocities Relativistic Energy and E= mc 2
Chapter 9 Relativeity Chapter Outline 9-1 The Postulate t of Speial Relativity it 9- The Relativity of Time and Time Dilation 9-3 The Relativity of Length and Length Contration 9-4 The Relativisti Addition
Experiment 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,
fiziks Institute for NET/JRF, GATE, IIT JAM, JEST, TIFR and GRE in PHYSICAL SCIENCES CLASSICAL MECHANICS SOLUTIONS
fizis CLASSICAL MECHANICS SOLUTIONS GATE- Q. For the set of all Lorentz transforations with eloities along the x-axis onsider the two stateents gien below: P: If L is a Lorentz transforation then, L -
PHYSICS. Time allowed: 90 minutes. Section A is a set of questions on data analysis. It requires work on graph paper.
PHYSICS EXAMIATIO FOR ETRACE SCHOLARSHIPS JAUARY 7 Tie allowed: 9 inutes Section A is a set of questions on data analysis. It equies wok on gaph pape. Section B consists of nine questions. Attept as any
Reflectance 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:
Practice Integration Math 120 Calculus I Fall 2015
Pactice Integation Math 0 Calculus I Fall 05 Hee s a list of pactice eecises. Thee s a hint fo each one as well as an answe with intemediate steps... ( + d. Hint. Answe. ( 8 t + t + This fist set of indefinite
Chapter 8. Linear Momentum, Impulse, and Collisions
Chapte 8 Lnea oentu, Ipulse, and Collsons 8. Lnea oentu and Ipulse The lnea oentu p of a patcle of ass ovng wth velocty v s defned as: p " v ote that p s a vecto that ponts n the sae decton as the velocty
Journal of Theoretics Vol.4-4
Journal of Theoretis ol.4-4 Cherenko s Partiles as Magnetons Dipl. Ing. Andrija Radoić Nike Strugara 3a, 3 Beograd, Yugoslaia Eail: andrijar@eunet.yu Abstrat: The artile will show that the forula for Cherenko
Answers 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
Practice Integration Math 120 Calculus I D Joyce, Fall 2013
Pactice Integation Math 0 Calculus I D Joyce, Fall 0 This fist set of indefinite integals, that is, antideivatives, only depends on a few pinciples of integation, the fist being that integation is invese
( ) rad ( 2.0 s) = 168 rad
.) α 0.450 ω o 0 and ω 8.00 ω αt + ω o o t ω ω o α HO 9 Solution 8.00 0 0.450 7.8 b.) ω ω o + αδθ o Δθ ω 8.00 0 ω o α 0.450 7. o Δθ 7. ev.3 ev π.) ω o.50, α 0.300, Δθ 3.50 ev π 7π ev ω ω o + αδθ o ω ω
AP Physics Electric Potential Energy
AP Physics lectic Potential negy Review of some vital peviously coveed mateial. The impotance of the ealie concepts will be made clea as we poceed. Wok takes place when a foce acts ove a distance. W F
Torque, Angular Momentum and Rotational Kinetic Energy
Toque, Angula Moentu and Rotational Kinetic Enegy In ou peious exaples that inoled a wheel, like fo exaple a pulley we wee always caeful to specify that fo the puposes of the poble it would be teated as
Electric Charge and Field
lectic Chage and ield Chapte 6 (Giancoli) All sections ecept 6.0 (Gauss s law) Compaison between the lectic and the Gavitational foces Both have long ange, The electic chage of an object plas the same
Physics 6C. Special Relativity. Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB
Physis 6C Speial Relatiity Two Main Ideas The Postulates of Speial Relatiity Light traels at the same speed in all inertial referene frames. Laws of physis yield idential results in all inertial referene
COMPARING 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
Electrostatics. 1. Show does the force between two point charges change if the dielectric constant of the medium in which they are kept increase?
Electostatics 1. Show does the foce between two point chages change if the dielectic constant of the medium in which they ae kept incease? 2. A chaged od P attacts od R whee as P epels anothe chaged od
PHYS 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
The Geometric Concept of Matter
The Geoeti Conept of Matte Zoan Ozie * Mah 5, 008 A B S T R A C T The geoeti onept of atte efines the funaental stutue of the eleentay ateial patile as a otating-ibating sphee. All the essential popeties
Unit 6 Practice Test. Which vector diagram correctly shows the change in velocity Δv of the mass during this time? (1) (1) A. Energy KE.
Unit 6 actice Test 1. Which one of the following gaphs best epesents the aiation of the kinetic enegy, KE, and of the gaitational potential enegy, GE, of an obiting satellite with its distance fom the
Time Dilation as Field
Jounal of Moden hysis 0 3 00-07 http://dx.doi.og/0.436/jmp.0.307 ublished Online Febuay 0 (http://www.si.og/jounal/jmp) Time Dilation as Field iot Ogonowski Wasaw oland Email: piot.ogonowski@piotogonowski.pl
E(r,t) = e 3. r 3. (b) Show that the transverse current, J t,is 3n(n e 3 ) e 3
Polem Set 3 (Jakson 6.20).. An example of the pesevation of ausality and finite speed of popagation in spite of the use of the Coulomg gauge is affoded y a unit stength dipole soue that is flashed on and
Version 1.0. klm. General Certificate of Education June Mathematics. Mechanics 2B. Mark Scheme
Vesion.0 klm Geneal Cetificate of Education June 00 Mathematics MMB Mechanics B Mak Scheme Mak schemes ae pepaed by the Pincipal Examine and consideed, togethe with the eleant questions, by a panel of
Newton s E = mc 2 Two Hundred Years Before Einstein? Newton = Einstein at the Quantum Scale
Newton s E = Two Hunded Yeas Befoe Einstein? Newton = Einstein at the Quantu Scale Espen Gaade Haug Nowegian Uniesity of Life Sciences August 7, 07 Abstact The ost faous Einstein foula is E =, while Newton
Journal of Theoretics
Jounal of Theoetis Volume 6-1, Feb-Mah 4 An Altenative Exlanation of the Cosmologial Redshift by the Tahyon Plasma Field in Integalati Sae Takaaki Musha musha@jda-tdi.go.j, musha@jg.ejnet.ne.j MRI, -11-7-61,
Section 11. Timescales Radiation transport in stars
Section 11 Timescales 11.1 Radiation tanspot in stas Deep inside stas the adiation eld is vey close to black body. Fo a black-body distibution the photon numbe density at tempeatue T is given by n = 2
CHEM1101 Worksheet 3: The Energy Levels Of Electrons
CHEM1101 Woksheet 3: The Enegy Levels Of Electons Model 1: Two chaged Paticles Sepaated by a Distance Accoding to Coulomb, the potential enegy of two stationay paticles with chages q 1 and q 2 sepaated
Physics 121 Hour Exam #5 Solution
Physics 2 Hou xam # Solution This exam consists of a five poblems on five pages. Point values ae given with each poblem. They add up to 99 points; you will get fee point to make a total of. In any given
Time Dilation in Gravity Wells
Time Dilation in Gavity Wells By Rihad R. Shiffman Digital Gaphis Asso. 038 Dunkik Ave. L.A., Ca. 9005 s@isi.edu This doument disusses the geneal elativisti effet of time dilation aused by a spheially
What is the length of the pendulum? Period = T = 12.0 s
Eaple: hen visitin an office buildin you notice that it has an atiu with an enoous pendulu with one end attached to the oof of the buildin and the othe end nealy eachin the floo. You obseve that the pendulu
Eddy 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
The Special Theory of Relativity
The Speial Theory of Relatiity Galilean Newtonian Relatiity Galileo Galilei Isaa Newton Definition of an inertial referene frame: One in whih Newton s first law is alid. onstant if F0 Earth is rotating
Force & Motion: Newton s Laws
oce & otion: Newton Law ( t Law) If no net foce act on a body then the body velocity cannot change. Zeo net foce implie zeo acceleation. The ma of an object detemine how difficult it i to change the object
Physics 202, Lecture 2
Physics 202, Lectue 2 Todays Topics Electic Foce and Electic Fields Electic Chages and Electic Foces Coulomb's Law Physical Field The Electic Field Electic Field Lines Motion of Chaged Paticle in Electic
Derivation of Non-Einsteinian Relativistic Equations from Momentum Conservation Law
Asian Journal of Applied Siene and Engineering, Volue, No 1/13 ISSN 35-915X(p); 37-9584(e) Derivation of Non-Einsteinian Relativisti Equations fro Moentu Conservation Law M.O.G. Talukder Varendra University,
Chapter 3. Problem Solutions
Capter. Proble Solutions. A poton and a partile ave te sae wavelengt. Can anyting be said about ow teir linear oenta opare? About ow te poton's energy opares wit te partile's total energy? About ow te
Physics 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.
Electromagnetic Waves
Eletroagneti Waves Physis 6C Eletroagneti (EM) waves an be produed by atoi transitions (ore on this later), or by an alternating urrent in a wire. As the harges in the wire osillate bak and forth, the
Errors in Nobel Prize for Physics (3) Conservation of Energy Leads to Probability Conservation of Parity, Momentum and so on
Eos in Nobel ize fo hysics (3) Conseation of Enegy Leads to obability Conseation of aity, Momentum and so on Fu Yuhua (CNOOC Reseach Institute, E-mail:fuyh945@sina.com) Abstact: One of the easons fo 957
Physics 1501 Lecture 19
Physcs 1501 ectue 19 Physcs 1501: ectue 19 Today s Agenda Announceents HW#7: due Oct. 1 Mdte 1: aveage 45 % Topcs otatonal Kneatcs otatonal Enegy Moents of Ineta Physcs 1501: ectue 19, Pg 1 Suay (wth copason
(conservation of momentum)
Dynamis of Binay Collisions Assumptions fo elasti ollisions: a) Eletially neutal moleules fo whih the foe between moleules depends only on the distane between thei entes. b) No intehange between tanslational
You are to turn in this final and the scantron to the front when finished.
Physics Fall 00: Final Exa Vesion B Nae: Quiz Code Nube: Closed book. No wok needs to be shown fo ultiple-choice questions.. Conside a ass on a sping that is undegoing siple haonic otion. In this siple
Content 5.1 Angular displacement and angular velocity 5.2 Centripetal acceleration 5.3 Centripetal force. 5. Circular motion.
5. Cicula otion By Liew Sau oh Content 5.1 Angula diplaceent and angula elocity 5. Centipetal acceleation 5.3 Centipetal foce Objectie a) expe angula diplaceent in adian b) define angula elocity and peiod
( ) Physics 1401 Homework Solutions - Walker, Chapter 9
Phyic 40 Conceptual Quetion CQ No Fo exaple, ey likely thee will be oe peanent deoation o the ca In thi cae, oe o the kinetic enegy that the two ca had beoe the colliion goe into wok that each ca doe on
anubhavclasses.wordpress.com CBSE Solved Test Papers PHYSICS Class XII Chapter : Electrostatics
CBS Solved Test Papes PHYSICS Class XII Chapte : lectostatics CBS TST PAPR-01 CLASS - XII PHYSICS (Unit lectostatics) 1. Show does the foce between two point chages change if the dielectic constant of
Voltage ( = Electric Potential )
V-1 of 10 Voltage ( = lectic Potential ) An electic chage altes the space aound it. Thoughout the space aound evey chage is a vecto thing called the electic field. Also filling the space aound evey chage
Physics 30 Lesson 20 Magnetic Forces Charged Particles
Physics 30 Lesson 20 Magnetic Foces Chaged Paticles I. Chaged paticles in extenal agnetic fields In the pevious lesson we leaned that when a chaged paticle is in otion, a agnetic field is induced aound
Autodesk Robot Structural Analysis Professional - Verification Manual for Italian Codes
Autodesk Robot Stutual Analysis Pofessional VERIFICATIO MAUAL FOR ITALIA CODES Mah 2014 ITRODUCTIO... 1 COCRETE... 2 1. DM 9/1/96 RC COLUMS... 3 VERIFICATIO EXAMPLE 1 - COLUM SUBJECTED TO AXIAL LOAD AD
Electricity Revision ELECTRICITY REVISION KEY CONCEPTS TERMINOLOGY & DEFINITION. Physical Sciences X-Sheets
Electicity Revision KEY CONCEPTS In this session we will focus on the following: Stating and apply Coulomb s Law. Defining electical field stength and applying the deived equations. Dawing electical field
The Radii of Baryons
Jounal Heading Yea; Vol. (No.): page ange DOI: 0.592/j.xxx.xxxxxxxx.xx The Radii of Bayons Maio Evealdo de Souza Depatmento de Físia, Univesidade Fedeal de Segipe, São Cistovão, 4900-000, Bazil Astat Consideing
2/24/2014. The point mass. Impulse for a single collision The impulse of a force is a vector. The Center of Mass. System of particles
/4/04 Chapte 7 Lnea oentu Lnea oentu of a Sngle Patcle Lnea oentu: p υ It s a easue of the patcle s oton It s a vecto, sla to the veloct p υ p υ p υ z z p It also depends on the ass of the object, sla
Orbital 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
TAP 702-6: Binary stars
TAP 702-6: Binary stars Orbiting binary stars: A type of ariable star. This type of ariable star onsists of two stars orbiting around eah other. When the dier star is in front of the brighter one, the
When a mass moves because of a force, we can define several types of problem.
Mechanics Lectue 4 3D Foces, gadient opeato, momentum 3D Foces When a mass moves because of a foce, we can define seveal types of poblem. ) When we know the foce F as a function of time t, F=F(t). ) When
Homework Set 4 Physics 319 Classical Mechanics. m m k. x, x, x, x T U x x x x l 2. x x x x. x x x x
Poble 78 a) The agangian i Hoewok Set 4 Phyic 319 Claical Mechanic k b) In te of the cente of a cooinate an x x1 x x1 x xc x x x x x1 xc x xc x x x x x1 xc x xc x, x, x, x T U x x x x l 1 1 1 1 1 1 1 1
KIRCHHOFF CURRENT LAW
KICHHOFF CUENT LAW ONE OF THE FUNDAMENTAL CONSEATION PINCIPLES IN ELECTICAL ENGINEEING CHAGE CANNOT BE CEATED NO DESTOYED NODES, BANCHES, LOOPS A NODE CONNECTS SEEAL COMPONENTS. BUT IT DOES NOT HOLD ANY
e sin cos i sin sin j cos k [2 POINTS] (c) Hence, determine expressions for sin sin i sin cos j sin e
![e sin cos i sin sin j cos k [2 POINTS] (c) Hence, determine expressions for sin sin i sin cos j sin e](/thumbs/84/89549943.jpg "e sin cos i sin sin j cos k [2 POINTS] (c) Hence, determine expressions for sin sin i sin cos j sin e")
EN: Continuum Mehanis Homewok : Kinematis Due : noon Fiday Febuay 4th Shool of Engineeing Bown Univesity. To analyze the defomation of a onial membane, it is poposed to use a two-dimensional onial-pola
Revised Newtonian Formula of Gravity and Equation of Cosmology in Flat Space-Time Transformed from Schwarzschild Solution
Intenational Jounal of Astonomy and Astophysis,,, 6-8 http://dx.doi.og/.46/ijaa.. Published Online Mah (http://www.sip.og/jounal/ijaa) evised Newtonian Fomula of Gavity and Equation of Cosmology in Flat
Extra 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
Chapter 39 Relativity
Chapter 39 Relatiity from relatie motion to relatiity 39. The Priniple of Galilean Relatiity The laws of mehanis mst be the same in all inertial frames of referene. Galilean spae-time transformation eqations
Work, Energy and Momentum
Work, Energy and Moentu Work: When a body oves a distance d along straight line, while acted on by a constant force of agnitude F in the sae direction as the otion, the work done by the force is tered
FZX: Personal Lecture Notes from Daniel W. Koon St. Lawrence University Physics Department CHAPTER 7
FZX: Pesonal Lectue Notes fom Daniel W. Koon St. Lawence Univesity Physics Depatment CHAPTER 7 Please epot any glitches, bugs o eos to the autho: dkoon at stlawu.edu. 7. Momentum and Impulse Impulse page
Ion-sound waves (electrostatic low frequency waves)
OTHER TYPES of WAVES Ion-sound waves (eletostati low fequeny waves) ae longitudinal waves simila lassial sound in gas s kt k M B plasma sound is slow fo eletons, but fast fo ions Eleton density is in eah
CHAPTER 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