F (-4.32x x10 k) Newtons a = (-4.742x x10 )m/s 9.11x10 kg

Size: px
Start display at page:

Download "F (-4.32x x10 k) Newtons a = (-4.742x x10 )m/s 9.11x10 kg"

Transcription

1 P Physics d Quate Test Review KEY k 8.99 x 9 Nm /C 8.85 x - C /Nm e.6 x -9 C milli - mico -6 nano -9 pico - Mega 6 Electostatics. Chage, Field, and Potential a. poton is placed in a unifom electic field that has a value of (.i.5j) Newtons/Coulomb. What is the foce on the poton? F E (.6 x -9 C) (.i.5j) (4.8 x -9 i 4. x -9 j) Newtons b. n electon is placed at (.,., -.5) m. The electic field in that aea is given by the function E (.(N/Cm )x i.5(n/cm )y k) Newtons/Coulomb. What is the foce on the paticle? E() i.5() k (7i k) N/C F E (-.6 x -9 C) (7i k) N/C (-4. x -8 i. x -8 k) Newtons c. dipole has a moment of 6.7 x - j Coulomb-metes. It is placed in a unifom field (.i.5j) Newtons/Coulomb. Find the initial foce, toue, & potential enegy on the dipole. ΣF τ p x E (6.7 x - j) x (.i) -. k Nm U - p E -(6.7 x - j) (-.5j).68 J d. Indicate on the diagam below whee the electic field is stongest and whee it is the weakest. weak stong What is the diffeence between electic field lines and electic field vectos? Field lines stat at the chage and use density to show magnitude. Vectos stat at the point whee field is evaluated & use length to show magnitude. Daw field lines fo the non-conducting sheet of chage below. _ e. Calculate the initial acceleation of the electon in #b F (-4.x.x k) Newtons a (-4.74x.5x )m/s - m i 9.x kg i k

2 f. poton is initially taveling at a speed of.x 5 m/s when it entes a unifom field of 5. V/m. What is the final speed of the poton if it tavels. mm though this field? V Ed (5 V / m)(. m).5v 9 W V (.6x C)(.5 V ).4x J W K m v v v f ( f i ) ( x J) 7 5 W mv.4 (.67x kg)(x m / s) i, 5 m / s 7 m (.67x kg) g. Electic potentials ae dawn fo an electic field in the diagam below. Is the field unifom? yes o no (cicle one) Explain you answe. The euipotential sufaces ae evenly spaced. What is the diection of the field? left h. If a. C chage has. kj of kinetic enegy at point, how much kinetic enegy will the. C chage have when it eaches point. W K K W K V K ( C)( V ), J 9, 4J f i i i. If the function fo electic field is given by.x.x 5., find a function fo the potential at any point in the field. V E dx x x 5dx x x 5x C j. If the function fo potential is given by 5.xy.z, find the electic field stength at (.,. -.) m. E E x y V 5 V V 5 V V 5 V V 5yi 5i x V 5xj j y V Ez 6zk 6k z E ( 5i j 6 k) V / m

3 . Coulomb s aw and Field and Potential of Point Chages a. Find the foce on the bottom ight chage. Each chage is -. C. P. m tanθ 4 θ 6.6 F k( C) ( m) ( (4 m) ( m) ).,7 x N k( C) F x N 9 4.5, 6.6 k( C) 9 F4 5.6x N, (4 m) i j 8 9 F.7x N, 68.5 (8.68x.x ) N b. Point P is located at the cente of the ectangle above. Detemine the potential at point P due to all 4 chages. n ki 4 k( C) V 4.8 i i ( m) ( m) x V c. How much wok must be applied to bing a 5. Coulomb chage fom infinity to point P in the ectangle above? Wapplied V (5 C)(-4.8 x V V) -.4 x J d. Calculate the total electical potential enegy of the five chage system, afte the 5. Coulomb chage is placed at point P. U Wapplied -.4 x J o you could add up each combination of U U U 4. m Uf.4x J k( C) 8.7x J U k 4 4 f i.4x J k( C)

4 z.5 m. Fields and Potentials of Othe Chage Distibutions a. Find the potential at point P (diectly above the left end of the line of chage) due to the unifom line of chage. The line of chage has a total chage of 7. C and a length of. m. Its thickness is negligible. P θ x dx x kd V d Q dx Q d dx kq dx V x z kq V x x x tanθ z x z tanθ dx z sec θdθ dx x z x z secθ z kq z sec θdθ kq z sec θdθ kq sec θdθ kq V z tan θ z z (tan θ ) secθ kq V u secθ tanθ du θ x x x x x x x x secθ tanθ kq x sec θ secθ tanθ secdθ dθ secθ tanθ x secθ tanθ x x θ θ dθ (sec sec tan ) secθdθ x x kq x du kq x kq x z x kq ln secθ tanθ ln ln( x z x) lnz x x u z z x x V kq V kq ln( z ) lnz lnz lnz ln( z ) lnz k(7 C) ln( ( ) (.5 ) ( )) ln(.5 ) 5. V m m m m x V ( m) 4

5 decosθ b. Find the electic field and potential at point P that is.5 m above a ing of chage. Point P lies on the cental axis of the ing of chage. The total chage of the ing is. micocoulombs. The adius of the ing is. m. desinθ d k E k d cosθ de R z Θ z P cosθ R z k z kz Qkz E d d R z R z Θ z ( µ C) k(.5 m) E,95 V / m ((. m) (.5 m) ) ( R z ) ( R z ) d k k( µ C) V k 7, 6V R z (. m) (.5 m) R R 5

6 c. P Find the electic field and potential at point P that is.5 m above a unifom disk of chage. Point P lies on the cental axis of the disk of chage. The total chage of the ing is 5. micocoulombs. The adius of the ing is.m. d z R ( z R z) Q (5 µ C) σ.59x C / m π π (. m) d σd σ πd 4 zd zσ πd de 4 π ( ) 4 ( ) z R π z R σz R d E 4 ( z ) u z du d σz R du σz u E 4 4 / ( u) R E (.5m) (.m) fom electic field fo single ing σz σ z z R z z R 4.59x C / m.5m 5.75 / d σd σ πr ' dr ' σ R' R πr ' dr ' 4π ' 4π 4π 4 π R z R ' V u z R ' du R ' dr ' R' R σ σ σ σ V u u 4 4 ' R R R R' Rdu ' z R ' R' u R' σ.59x C / m V 4 R' ( ) (.5 ) (. ) (.5 ) 8.9 x V m 4 m m m x V d. Daw field lines fo a set of paallel plates e. Daw field lines fo a long unifomly chaged wie o thin cylindical shell. Use a coss-sectional view. 6

7 f. Daw field lines fo a thin spheical shell. Use a coss-sectional view. 4. Gauss aw a. non-unifom electic field given by E (.x)i (.5y y)j (.z )k pieces the Gaussian cube shown below. The back bottom left vetex of the cube is located at the oigin. The cube has a side length of. m. Detemine the electic flux though each face and the total flux though the cube. y m font Φ E Φ k k Φ back ight Φ left top Φ bottom ( ). / x Φ i i.(). / Φ j j Φ (.5( ) ).5 / 7.7 / Nm C Nm C Nm C Nm C z b. egin with Gauss law and deive an expession fo the electic field at a point a distance of fom a unifomly chaged infinitely long thin wie. The wie has a linea chage density of λ. Include a elevant sketch. Eπl λl E d enclosed λ E π 7

8 c. The diagam below shows a spheical shell made of pocelain, i.e., it is non-conducting. Chage is unifomly distibuted thoughout the shell. Find an expession fo the electic field fo <a, fo a<<b, and fo >b. Make a plot of vs. b. ssume the total chage on the shell is Q. a b E a b fo <a E E d fo a<<b ρ 4 ( b a ) π E π E 4 π ( a ) fo >b E d Q ( a ) 4 π ( b a ) E4 Q π Q E 4π Q E d enclosed enclosed Q 4 4 π ( b a ) enclosed d. Find the suface chage density of the conducting sheet of chage below. ssume that the sheet is vey lage compaed to the small -. micocoulomb chage suspended with a non-conducting sting. The -. micocoulomb chage has a mass of. milligams. ssume eveything is at est. E mg T F y T cosθ mg mg T cosθ F x T sinθ E σ mg tanθ mg tanθ σ 6 (x kg) g tan σ 5 pc / m ( µ C) Note: mg -6 kg 8

9 Conductos, Capacitos, and Dielectics 5. Electostatics with Conductos a. Give at least two possible explanations fo why thee is no chage inside a conducto. Chage edistibutes to make like chages fa away fom each othe. If thee was chage on the inside, thee would be field. This would cause the chages to be in pepetual motion. b. Why is a conducto an euipotential suface? Othewise, chage would constantly be in motion on the suface. c. In the diagam below, the sphee on the left,, initially has a adius of.5 mm and a chage of. nc. The sphee on the ight, has a adius of. mm and a chage of 5. nc. The sphees ae. metes apat. Find the net chage on each sphee, afte they ae connected with a conducting wie. d. 5. pf chage is bought nea a lage non-conducting sheet of chage that has a chage density of 5. µc/m. If the 5. pf chage has a mass of. µg, calculate its acceleation. σ F ma E σ (5 pf)(5 µ C / m ) a 47 m / s m (x kg) 9 Note: µ 9 g x kg V V k k.5 mm.mm 5nC.5. 5 e. On the gaph below, make a sketch of V vs. fo a conducting sphee with a adius R and chage Q. abel impotant points. fo <R: VkQ/R fo >R: VkQ/ V kq/r nc nc R 9

10 6. Capacitos a. paallel plate capacito has an aea. x -4 m and a plate sepaation d. mm. Find its capacitance. 4 (x m ) C.77pF d (x m) b. If the capacito above is then connected to a. V battey, what is the chage on the capacito? CV (.77 pf)( V ).pc c. How much enegy is stoed in the above capacito when it is fully chaged? (.77 )( ).7 U CV pf V nj d. The battey is disconnected and a.8 mm slab of pocelain is inseted between the plates of the capacito. Calculate the electic field in the slab of pocelain. σ.pc E 846 V / m κ κ 6.5(x m ) 4 e. Calculate the electic field in the ai gaps between the capacito plates. E σ κ(846 V / m), V / m f. Calculate the potential diffeence acoss the capacito. V Ed (846 V / m)(.8x m) (, V / m)(.x m).88v g. Calculate the new capacitance..pc c 5.5pF V.88V h. If the battey had not been disconnected, the chage stoed on the capacito would have changed. What would the new chage be? CV (5.5 pf)( V ) 66pC i. Calculate the wok applied when the dielectic was inseted. (5.5 )( ).7.69 Wapplied U pf V nj nj j. The oute adius of a cylindical capacito is inceased while the capacito is connected to a battey. How will the chage change? C π and CV ln( b / a) b C

11 k. The oute adius of a spheical capacito is inceased while the capacito is connected to a battey. How will the chage change? ab a C 4 π 4 π and CV b a a / b b C i. Find the euivalent capacitance of the cicuit below. C. µf, C 4. µf, and C 5. µf. CC ( µ F)(4 µ F) Ce C 5µ F 6.7µ F C C µ F 4µ F j. In the cicuit below, the esisto R 6Ω, the emf is V, and the capacito C. nf. Find the cuent in the cicuit when the switch is fist placed at a. V V i. R 6Ω k. Find the cuent in the cicuit above, a long time afte the switch is in position a. i l. What is the maximum chage on the capacito above? CV ( nf)( V ) 6nC

12 m. How long does it take fo the capacito above to each half its maximum chage? Q CV e t / RC ( ) CV CV e t / RC e t / RC e ln t / RC t / RC ( ) t RC Ω nf x 5 ln ln (6 )( ). sec n. fte a long time, the switch is flipped to position b. Calculate the initial cuent. i-. (opposite diection of the initial cuent when the switch is flipped to a). o. What is the cuent a long time afte the switch is flipped to position b. i p. What is the time constant of the cicuit? RC Ω nf x Electic Cicuits 5 (6 )( ).8 sec 7. Cuent, Resistance, Powe a. If thee is a cuent of 5. in a esisto, how much chage passes though the esisto in. hous? 5C 6s i t h( )( ) 6C s h b. What is the potential diffeence acoss the above esisto, if it has a esistance of 5. Ω? V ir (5 )(5 Ω ) 5V c. conducto of a unifom adius. cm caies a cuent of. poduced by an electic field of V/m. What is the esistivity of the mateial? ρ ( m) E E Eπ ( V / m) π. J i / i.8x Ω d. Detemine the esistance of a cylindical esisto at K that is made of silve and has a adius of 5. mm. The esisto is. cm long. fom p. 669, ρ.6x Ωm and α 4.x K R 8 - ρ ρ ρα Ω Ω Ω ( T T ).6x m (.6x m)(4.x K )(K 9 K).67x m x Ωm m π (.5 m) 8 ρ (.67 )(. ) 6.x Ω m

13 e. n electic heate is constucted by applying a potential diffeence of V to a nichome wie of total esistance 8. Ω. Find the cuent caied by the wie and the powe ating of the heate. V ( V ) P 5W R 8Ω V V i.75 R 8Ω f. On the cicuit below, indicate how you would connect an ammete and a voltmete to ead the cuent and voltage espectively, in R. i i V i g. Given the values of E. V, E 4. V, E 9. V, R 6. Ω, and R. Ω, detemine the cuent in each banch of the cicuit. i i i i i i ξ ir ir ξ ir i i 4 i i ξ ir ir ξ ir 4 i i 9 i i 5 i i i i i i ampees.97

14 h. Find the euivalent esistance of the netwok shown below. Re R R R R R R RRR 4 RR 4 RR 4 RR RR 4 RR 4 RR 4 4 RRR i. Explain why the esistance of an ammete must be low. If it was high, it would dastically educe the cicuit cuent since ammetes ae connected in seies. k. Explain why the esistance of a voltmete must be high. If it was low, moe of the cuent would be diveted fom the tested banch. This would alte the value of the potential dop. 4

15 6.7Ω i E i C i i D 6.7Ω.7Ω i F.7Ω l. In the cicuit above, R. Ω, R. Ω, R. Ω, R4 4. Ω, R5 5. Ω, R6 6. Ω, R7 7. Ω. R8 8. Ω, E. V, and E. V. Find the value i and i. loop : V 9iD V id to calculate i, detemine the euivalent esistance fo all esistos to the left of E (see diagam) V i.6 6.7Ω junction : i ic id ic.6 loop : 6i ic-v i (-(.6))/6.86 junction: ie ic- i loop: 8i 7iF junction : ie i if.76 i(8/7)i i.6 5

16 R m. battey has an emf of 5. V. The teminal voltage of the battey is.6 V when it is deliveing. W of powe to an extenal load esisto R. What is the value of R? V P R V (.6 V ) R 6.7Ω P W n. In the above poblem, what is the intenal esistance of the battey? V.6V i.7 R 6.7Ω V ξ i.6v 5 V (.7 ).97Ω Magnetostatics 8. Foces on Moving Chages in Magnetic Fields a. Explain why a magnetic field cannot do wok. Magnetic fields cannot do wok because the foce they exet is always pependicula to the displacement. b. n electon moving along the positive x axis pependicula to a magnetic field expeiences a magnetic deflection in the negative y diection. What is the diection of the magnetic field? -z c. n electon is pojected into a unifom magnetic field (.4i.j) T. Find the vecto expession fo the foce on the electon when its velocity v.7 x 5 j m/s. Fvx (-.6x -9 C)(-.7x 5 jm/s x.4i) -8.9x -4 k Newtons d. poton is moving in a cicula obit of adius 4 cm in a unifom magnetic field of magnitude.5 T diected pependicula to the velocity of the poton. Find the obital speed of the poton. F ma v v m 9 (.6x C)(.5 T )(.4 m) v 7 m (.67x kg) / x m s 6

17 e. cossed field velocity selecto has a magnetic field of magnitude. T. What electic field stength is euied if. kev electons ae to pass though undeflected? K mv 9.6x J (, ev ) (9.x kg) v ev v E / F F E v x m s 7 5 E v (5.9x m / s)(. T ) 5.9x V / m 9. Foces on Cuent Caying Wies in Magnetic Fields a. wie having a mass pe unit length of.5 g/cm caies a. cuent hoizontally to the south. What ae the diection and magnitude of the minimum magnetic field needed to lift this wie vetically upwad? West.5g kg cm.5kg cm g m m F mg il mg mg.5 kg (9.8 m / s ).45T li m b. cuent of 7. m is maintained in a single cicula loop of. m cicumfeence. unifom magnetic field of.8 T is diected paallel to the plane of the loop. Calculate the magnetic moment of the loop. πd.m d. m / π.64m π (.64 m) µ Ni ()(7x ) 5.4x m 4 c. What is the magnitude of the toue exeted on the loop in the above poblem by the magnetic field when the plane of the loop is paallel to the magnetic field? τ µx (5.4x m )(.8 T ) 4.x Tm 7

Phys102 Second Major-182 Zero Version Monday, March 25, 2019 Page: 1

Phys102 Second Major-182 Zero Version Monday, March 25, 2019 Page: 1 Monday, Mach 5, 019 Page: 1 Q1. Figue 1 shows thee pais of identical conducting sphees that ae to be touched togethe and then sepaated. The initial chages on them befoe the touch ae indicated. Rank the

More information

ev dm e evd 2 m e 1 2 ev2 B) e 2 0 dm e D) m e

ev dm e evd 2 m e 1 2 ev2 B) e 2 0 dm e D) m e . A paallel-plate capacito has sepaation d. The potential diffeence between the plates is V. If an electon with chage e and mass m e is eleased fom est fom the negative plate, its speed when it eaches

More information

Physics 313 Practice Test Page 1. University Physics III Practice Test II

Physics 313 Practice Test Page 1. University Physics III Practice Test II Physics 313 Pactice Test Page 1 Univesity Physics III Pactice Test II This pactice test should give you a ough idea of the fomat and oveall level of the Physics 313 exams. The actual exams will have diffeent

More information

ELECTROSTATICS::BHSEC MCQ 1. A. B. C. D.

ELECTROSTATICS::BHSEC MCQ 1. A. B. C. D. ELETROSTATIS::BHSE 9-4 MQ. A moving electic chage poduces A. electic field only. B. magnetic field only.. both electic field and magnetic field. D. neithe of these two fields.. both electic field and magnetic

More information

Potential Energy. The change U in the potential energy. is defined to equal to the negative of the work. done by a conservative force

Potential Energy. The change U in the potential energy. is defined to equal to the negative of the work. done by a conservative force Potential negy The change U in the potential enegy is defined to equal to the negative of the wok done by a consevative foce duing the shift fom an initial to a final state. U = U U = W F c = F c d Potential

More information

PHYS 1444 Section 501 Lecture #7

PHYS 1444 Section 501 Lecture #7 PHYS 1444 Section 51 Lectue #7 Wednesday, Feb. 8, 26 Equi-potential Lines and Sufaces Electic Potential Due to Electic Dipole E detemined fom V Electostatic Potential Enegy of a System of Chages Capacitos

More information

Phys 1215, First Test. September 20, minutes Name:

Phys 1215, First Test. September 20, minutes Name: Phys 115, Fist Test. Septembe 0, 011 50 minutes Name: Show all wok fo maximum cedit. Each poblem is woth 10 points. k =.0 x 10 N m / C ε 0 = 8.85 x 10-1 C / N m e = 1.60 x 10-1 C ρ = 1.68 x 10-8 Ω m fo

More information

18.1 Origin of Electricity 18.2 Charged Objects and Electric Force

18.1 Origin of Electricity 18.2 Charged Objects and Electric Force 1 18.1 Oigin of lecticity 18. Chaged Objects and lectic Foce Thee ae two kinds of electic chage: positive and negative. The SI unit of electic chage is the coulomb (C). The magnitude of the chage on an

More information

17.1 Electric Potential Energy. Equipotential Lines. PE = energy associated with an arrangement of objects that exert forces on each other

17.1 Electric Potential Energy. Equipotential Lines. PE = energy associated with an arrangement of objects that exert forces on each other Electic Potential Enegy, PE Units: Joules Electic Potential, Units: olts 17.1 Electic Potential Enegy Electic foce is a consevative foce and so we can assign an electic potential enegy (PE) to the system

More information

Physics 2212 GH Quiz #2 Solutions Spring 2016

Physics 2212 GH Quiz #2 Solutions Spring 2016 Physics 2212 GH Quiz #2 Solutions Sping 216 I. 17 points) Thee point chages, each caying a chage Q = +6. nc, ae placed on an equilateal tiangle of side length = 3. mm. An additional point chage, caying

More information

(Sample 3) Exam 1 - Physics Patel SPRING 1998 FORM CODE - A (solution key at end of exam)

(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 information

F = net force on the system (newton) F,F and F. = different forces working. E = Electric field strength (volt / meter)

F = net force on the system (newton) F,F and F. = different forces working. E = Electric field strength (volt / meter) All the Impotant Fomulae that a student should know fom. XII Physics Unit : CHAPTER - ELECTRIC CHARGES AND FIELD CHAPTER ELECTROSTATIC POTENTIAL AND CAPACITANCE S. Fomula No.. Quantization of chage Q =

More information

CHAPTER 25 ELECTRIC POTENTIAL

CHAPTER 25 ELECTRIC POTENTIAL CHPTE 5 ELECTIC POTENTIL Potential Diffeence and Electic Potential Conside a chaged paticle of chage in a egion of an electic field E. This filed exets an electic foce on the paticle given by F=E. When

More information

Calculate the electric potential at B d2=4 m Calculate the electric potential at A d1=3 m 3 m 3 m

Calculate the electric potential at B d2=4 m Calculate the electric potential at A d1=3 m 3 m 3 m MTE : Ch 13 5:3-7pm on Oct 31 ltenate Exams: Wed Ch 13 6:3pm-8:pm (people attending the altenate exam will not be allowed to go out of the oom while othes fom pevious exam ae still aound) Thu @ 9:-1:3

More information

Chapter 22: Electric Fields. 22-1: What is physics? General physics II (22102) Dr. Iyad SAADEDDIN. 22-2: The Electric Field (E)

Chapter 22: Electric Fields. 22-1: What is physics? General physics II (22102) Dr. Iyad SAADEDDIN. 22-2: The Electric Field (E) Geneal physics II (10) D. Iyad D. Iyad Chapte : lectic Fields In this chapte we will cove The lectic Field lectic Field Lines -: The lectic Field () lectic field exists in a egion of space suounding a

More information

15 B1 1. Figure 1. At what speed would the car have to travel for resonant oscillations to occur? Comment on your answer.

15 B1 1. Figure 1. At what speed would the car have to travel for resonant oscillations to occur? Comment on your answer. Kiangsu-Chekiang College (Shatin) F:EasteHolidaysAssignmentAns.doc Easte Holidays Assignment Answe Fom 6B Subject: Physics. (a) State the conditions fo a body to undego simple hamonic motion. ( mak) (a)

More information

CHAPTER 10 ELECTRIC POTENTIAL AND CAPACITANCE

CHAPTER 10 ELECTRIC POTENTIAL AND CAPACITANCE CHAPTER 0 ELECTRIC POTENTIAL AND CAPACITANCE ELECTRIC POTENTIAL AND CAPACITANCE 7 0. ELECTRIC POTENTIAL ENERGY Conside a chaged paticle of chage in a egion of an electic field E. This filed exets an electic

More information

PHYS 1444 Lecture #5

PHYS 1444 Lecture #5 Shot eview Chapte 24 PHYS 1444 Lectue #5 Tuesday June 19, 212 D. Andew Bandt Capacitos and Capacitance 1 Coulom s Law The Fomula QQ Q Q F 1 2 1 2 Fomula 2 2 F k A vecto quantity. Newtons Diection of electic

More information

Page 1 of 6 Physics II Exam 1 155 points Name Discussion day/time Pat I. Questions 110. 8 points each. Multiple choice: Fo full cedit, cicle only the coect answe. Fo half cedit, cicle the coect answe and

More information

SAMPLE PAPER I. Time Allowed : 3 hours Maximum Marks : 70

SAMPLE PAPER I. Time Allowed : 3 hours Maximum Marks : 70 SAMPL PAPR I Time Allowed : 3 hous Maximum Maks : 70 Note : Attempt All questions. Maks allotted to each question ae indicated against it. 1. The magnetic field lines fom closed cuves. Why? 1 2. What is

More information

PY208 Matter & Interactions Final Exam S2005

PY208 Matter & Interactions Final Exam S2005 PY Matte & Inteactions Final Exam S2005 Name (pint) Please cicle you lectue section below: 003 (Ramakishnan 11:20 AM) 004 (Clake 1:30 PM) 005 (Chabay 2:35 PM) When you tun in the test, including the fomula

More information

Algebra-based Physics II

Algebra-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 information

Review for Midterm-1

Review for Midterm-1 Review fo Midtem-1 Midtem-1! Wednesday Sept. 24th at 6pm Section 1 (the 4:10pm class) exam in BCC N130 (Business College) Section 2 (the 6:00pm class) exam in NR 158 (Natual Resouces) Allowed one sheet

More information

EM-2. 1 Coulomb s law, electric field, potential field, superposition q. Electric field of a point charge (1)

EM-2. 1 Coulomb s law, electric field, potential field, superposition q. Electric field of a point charge (1) EM- Coulomb s law, electic field, potential field, supeposition q ' Electic field of a point chage ( ') E( ) kq, whee k / 4 () ' Foce of q on a test chage e at position is ee( ) Electic potential O kq

More information

Phys 222 Sp 2009 Exam 1, Wed 18 Feb, 8-9:30pm Closed Book, Calculators allowed Each question is worth one point, answer all questions

Phys 222 Sp 2009 Exam 1, Wed 18 Feb, 8-9:30pm Closed Book, Calculators allowed Each question is worth one point, answer all questions Phys Sp 9 Exam, Wed 8 Feb, 8-9:3pm Closed Book, Calculatos allowed Each question is woth one point, answe all questions Fill in you Last Name, Middle initial, Fist Name You ID is the middle 9 digits on

More information

UNIT 3:Electrostatics

UNIT 3:Electrostatics The study of electic chages at est, the foces between them and the electic fields associated with them. UNIT 3:lectostatics S7 3. lectic Chages and Consevation of chages The electic chage has the following

More information

Physics 107 TUTORIAL ASSIGNMENT #8

Physics 107 TUTORIAL ASSIGNMENT #8 Physics 07 TUTORIAL ASSIGNMENT #8 Cutnell & Johnson, 7 th edition Chapte 8: Poblems 5,, 3, 39, 76 Chapte 9: Poblems 9, 0, 4, 5, 6 Chapte 8 5 Inteactive Solution 8.5 povides a model fo solving this type

More information

$ i. !((( dv vol. Physics 8.02 Quiz One Equations Fall q 1 q 2 r 2 C = 2 C! V 2 = Q 2 2C F = 4!" or. r ˆ = points from source q to observer

$ i. !((( dv vol. Physics 8.02 Quiz One Equations Fall q 1 q 2 r 2 C = 2 C! V 2 = Q 2 2C F = 4! or. r ˆ = points from source q to observer Physics 8.0 Quiz One Equations Fall 006 F = 1 4" o q 1 q = q q ˆ 3 4" o = E 4" o ˆ = points fom souce q to obseve 1 dq E = # ˆ 4" 0 V "## E "d A = Q inside closed suface o d A points fom inside to V =

More information

PHYS 2135 Exam I February 13, 2018

PHYS 2135 Exam I February 13, 2018 Exam Total /200 PHYS 2135 Exam I Febuay 13, 2018 Name: Recitation Section: Five multiple choice questions, 8 points each Choose the best o most nealy coect answe Fo questions 6-9, solutions must begin

More information

Prepared by: M. S. KumarSwamy, TGT(Maths) Page - 1 -

Prepared by: M. S. KumarSwamy, TGT(Maths) Page - 1 - Pepaed by: M. S. KumaSwamy, TGT(Maths) Page - - ELECTROSTATICS MARKS WEIGHTAGE 8 maks QUICK REVISION (Impotant Concepts & Fomulas) Chage Quantization: Chage is always in the fom of an integal multiple

More information

Electric Field, Potential Energy, & Voltage

Electric Field, Potential Energy, & Voltage Slide 1 / 66 lectic Field, Potential negy, & oltage Wok Slide 2 / 66 Q+ Q+ The foce changes as chages move towads each othe since the foce depends on the distance between the chages. s these two chages

More information

Objects usually are charged up through the transfer of electrons from one object to the other.

Objects usually are charged up through the transfer of electrons from one object to the other. 1 Pat 1: Electic Foce 1.1: Review of Vectos Review you vectos! You should know how to convet fom pola fom to component fom and vice vesa add and subtact vectos multiply vectos by scalas Find the esultant

More information

MAGNETIC FIELD INTRODUCTION

MAGNETIC FIELD INTRODUCTION MAGNETIC FIELD INTRODUCTION It was found when a magnet suspended fom its cente, it tends to line itself up in a noth-south diection (the compass needle). The noth end is called the Noth Pole (N-pole),

More information

Gauss s Law Simulation Activities

Gauss s Law Simulation Activities Gauss s Law Simulation Activities Name: Backgound: The electic field aound a point chage is found by: = kq/ 2 If thee ae multiple chages, the net field at any point is the vecto sum of the fields. Fo a

More information

Electrostatics (Electric Charges and Field) #2 2010

Electrostatics (Electric Charges and Field) #2 2010 Electic Field: The concept of electic field explains the action at a distance foce between two chaged paticles. Evey chage poduces a field aound it so that any othe chaged paticle expeiences a foce when

More information

1 2 U CV. K dq I dt J nqv d J V IR P VI

1 2 U CV. K dq I dt J nqv d J V IR P VI o 5 o T C T F 9 T K T o C 7.5 L L T V VT Q mct nct Q F V ml F V dq A H k TH TC dt L pv nt Kt nt CV ideal monatomic gas 5 CV ideal diatomic gas w/o vibation V W pdv V U Q W W Q e Q Q e Canot H C T T S C

More information

Current, Resistance and

Current, Resistance and Cuent, Resistance and Electomotive Foce Chapte 25 Octobe 2, 2012 Octobe 2, 2012 Physics 208 1 Leaning Goals The meaning of electic cuent, and how chages move in a conducto. What is meant by esistivity

More information

21 MAGNETIC FORCES AND MAGNETIC FIELDS

21 MAGNETIC FORCES AND MAGNETIC FIELDS CHAPTER 1 MAGNETIC ORCES AND MAGNETIC IELDS ANSWERS TO OCUS ON CONCEPTS QUESTIONS 1. (d) Right-Hand Rule No. 1 gives the diection of the magnetic foce as x fo both dawings A and. In dawing C, the velocity

More information

Exam 3, vers Physics Spring, 2003

Exam 3, vers Physics Spring, 2003 1 of 9 Exam 3, ves. 0001 - Physics 1120 - Sping, 2003 NAME Signatue Student ID # TA s Name(Cicle one): Michael Scheffestein, Chis Kelle, Paisa Seelungsawat Stating time of you Tues ecitation (wite time

More information

16.1 Permanent magnets

16.1 Permanent magnets Unit 16 Magnetism 161 Pemanent magnets 16 The magnetic foce on moving chage 163 The motion of chaged paticles in a magnetic field 164 The magnetic foce exeted on a cuent-caying wie 165 Cuent loops and

More information

Today in Physics 122: getting V from E

Today in Physics 122: getting V from E Today in Physics 1: getting V fom E When it s best to get V fom E, athe than vice vesa V within continuous chage distibutions Potential enegy of continuous chage distibutions Capacitance Potential enegy

More information

A) (0.46 î ) N B) (0.17 î ) N

A) (0.46 î ) N B) (0.17 î ) N Phys10 Secnd Maj-14 Ze Vesin Cdinat: xyz Thusday, Apil 3, 015 Page: 1 Q1. Thee chages, 1 = =.0 μc and Q = 4.0 μc, ae fixed in thei places as shwn in Figue 1. Find the net electstatic fce n Q due t 1 and.

More information

Physics 122, Fall September 2012

Physics 122, Fall September 2012 Physics 1, Fall 1 7 Septembe 1 Today in Physics 1: getting V fom E When it s best to get V fom E, athe than vice vesa V within continuous chage distibutions Potential enegy of continuous chage distibutions

More information

Flux. Area Vector. Flux of Electric Field. Gauss s Law

Flux. Area Vector. Flux of Electric Field. Gauss s Law Gauss s Law Flux Flux in Physics is used to two distinct ways. The fist meaning is the ate of flow, such as the amount of wate flowing in a ive, i.e. volume pe unit aea pe unit time. O, fo light, it is

More information

Objectives: After finishing this unit you should be able to:

Objectives: After finishing this unit you should be able to: lectic Field 7 Objectives: Afte finishing this unit you should be able to: Define the electic field and explain what detemines its magnitude and diection. Wite and apply fomulas fo the electic field intensity

More information

(r) = 1. Example: Electric Potential Energy. Summary. Potential due to a Group of Point Charges 9/10/12 1 R V(r) + + V(r) kq. Chapter 23.

(r) = 1. Example: Electric Potential Energy. Summary. Potential due to a Group of Point Charges 9/10/12 1 R V(r) + + V(r) kq. Chapter 23. Eample: Electic Potential Enegy What is the change in electical potential enegy of a eleased electon in the atmosphee when the electostatic foce fom the nea Eath s electic field (diected downwad) causes

More information

Electrostatics. 3) positive object: lack of electrons negative object: excess of electrons

Electrostatics. 3) positive object: lack of electrons negative object: excess of electrons Electostatics IB 12 1) electic chage: 2 types of electic chage: positive and negative 2) chaging by fiction: tansfe of electons fom one object to anothe 3) positive object: lack of electons negative object:

More information

Gauss Law. Physics 231 Lecture 2-1

Gauss Law. Physics 231 Lecture 2-1 Gauss Law Physics 31 Lectue -1 lectic Field Lines The numbe of field lines, also known as lines of foce, ae elated to stength of the electic field Moe appopiately it is the numbe of field lines cossing

More information

AP Physics Electric Potential Energy

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

More information

Chapter 23: GAUSS LAW 343

Chapter 23: GAUSS LAW 343 Chapte 23: GAUSS LAW 1 A total chage of 63 10 8 C is distibuted unifomly thoughout a 27-cm adius sphee The volume chage density is: A 37 10 7 C/m 3 B 69 10 6 C/m 3 C 69 10 6 C/m 2 D 25 10 4 C/m 3 76 10

More information

Chapter 22 The Electric Field II: Continuous Charge Distributions

Chapter 22 The Electric Field II: Continuous Charge Distributions Chapte The lectic Field II: Continuous Chage Distibutions A ing of adius a has a chage distibution on it that vaies as l(q) l sin q, as shown in Figue -9. (a) What is the diection of the electic field

More information

06 - ROTATIONAL MOTION Page 1 ( Answers at the end of all questions )

06 - ROTATIONAL MOTION Page 1 ( Answers at the end of all questions ) 06 - ROTATIONAL MOTION Page ) A body A of mass M while falling vetically downwads unde gavity beaks into two pats, a body B of mass ( / ) M and a body C of mass ( / ) M. The cente of mass of bodies B and

More information

Magnetic Field. Conference 6. Physics 102 General Physics II

Magnetic Field. Conference 6. Physics 102 General Physics II Physics 102 Confeence 6 Magnetic Field Confeence 6 Physics 102 Geneal Physics II Monday, Mach 3d, 2014 6.1 Quiz Poblem 6.1 Think about the magnetic field associated with an infinite, cuent caying wie.

More information

Electrostatics. 1. Show does the force between two point charges change if the dielectric constant of the medium in which they are kept increase?

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

More information

Electricity Revision ELECTRICITY REVISION KEY CONCEPTS TERMINOLOGY & DEFINITION. Physical Sciences X-Sheets

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

More information

Physics 11 Chapter 20: Electric Fields and Forces

Physics 11 Chapter 20: Electric Fields and Forces Physics Chapte 0: Electic Fields and Foces Yesteday is not ous to ecove, but tomoow is ous to win o lose. Lyndon B. Johnson When I am anxious it is because I am living in the futue. When I am depessed

More information

Review. Electrostatic. Dr. Ray Kwok SJSU

Review. Electrostatic. Dr. Ray Kwok SJSU Review Electostatic D. Ray Kwok SJSU Paty Balloons Coulomb s Law F e q q k 1 Coulomb foce o electical foce. (vecto) Be caeful on detemining the sign & diection. k 9 10 9 (N m / C ) k 1 4πε o k is the Coulomb

More information

Physics 122, Fall October 2012

Physics 122, Fall October 2012 Today in Physics 1: electostatics eview David Blaine takes the pactical potion of his electostatics midtem (Gawke). 11 Octobe 01 Physics 1, Fall 01 1 Electostatics As you have pobably noticed, electostatics

More information

Physics NYB problem set 5 solution

Physics NYB problem set 5 solution Physics NY poblem set 5 solutions 1 Physics NY poblem set 5 solution Hello eveybody, this is ED. Hi ED! ED is useful fo dawing the ight hand ule when you don t know how to daw. When you have a coss poduct

More information

Electo Magnetism iot Savat s Law and Ampee s Cicuital Law 1. A cuent is flowing due noth along a powe line. The diection of the magnetic field above it, neglecting the eath s field is: (1) Noth () East

More information

AP Physics C: Electricity and Magnetism 2003 Scoring Guidelines

AP Physics C: Electricity and Magnetism 2003 Scoring Guidelines AP Physics C: Electicity and Magnetism 3 Scoing Guidelines The mateials included in these files ae intended fo use by AP teaches fo couse and exam pepaation; pemission fo any othe use must be sought fom

More information

Advanced Subsidiary GCE (H157) Advanced GCE (H557) Physics B (Advancing Physics) Data, Formulae and Relationships Booklet

Advanced Subsidiary GCE (H157) Advanced GCE (H557) Physics B (Advancing Physics) Data, Formulae and Relationships Booklet Advanced Subsidiay GCE (H57) Advanced GCE (H557) Physics B (Advancing Physics) Data, Fomulae and Relationships Booklet The infomation in this booklet is fo the use of candidates following the Advanced

More information

ELECTROMAGNETISM (CP2)

ELECTROMAGNETISM (CP2) Revision Lectue on ELECTROMAGNETISM (CP) Electostatics Magnetostatics Induction EM Waves based on pevious yeas Pelims questions State Coulomb s Law. Show how E field may be defined. What is meant by E

More information

Force and Work: Reminder

Force and Work: Reminder Electic Potential Foce and Wok: Reminde Displacement d a: initial point b: final point Reminde fom Mechanics: Foce F if thee is a foce acting on an object (e.g. electic foce), this foce may do some wok

More information

Electromagnetism Physics 15b

Electromagnetism Physics 15b lectomagnetism Physics 15b Lectue #20 Dielectics lectic Dipoles Pucell 10.1 10.6 What We Did Last Time Plane wave solutions of Maxwell s equations = 0 sin(k ωt) B = B 0 sin(k ωt) ω = kc, 0 = B, 0 ˆk =

More information

A) N B) 0.0 N C) N D) N E) N

A) N B) 0.0 N C) N D) N E) N Cdinat: H Bahluli Sunday, Nvembe, 015 Page: 1 Q1. Five identical pint chages each with chage =10 nc ae lcated at the cnes f a egula hexagn, as shwn in Figue 1. Find the magnitude f the net electic fce

More information

EELE 3331 Electromagnetic I Chapter 4. Electrostatic fields. Islamic University of Gaza Electrical Engineering Department Dr.

EELE 3331 Electromagnetic I Chapter 4. Electrostatic fields. Islamic University of Gaza Electrical Engineering Department Dr. EELE 3331 Electomagnetic I Chapte 4 Electostatic fields Islamic Univesity of Gaza Electical Engineeing Depatment D. Talal Skaik 212 1 Electic Potential The Gavitational Analogy Moving an object upwad against

More information

Phys-272 Lecture 17. Motional Electromotive Force (emf) Induced Electric Fields Displacement Currents Maxwell s Equations

Phys-272 Lecture 17. Motional Electromotive Force (emf) Induced Electric Fields Displacement Currents Maxwell s Equations Phys-7 Lectue 17 Motional Electomotive Foce (emf) Induced Electic Fields Displacement Cuents Maxwell s Equations Fom Faaday's Law to Displacement Cuent AC geneato Magnetic Levitation Tain Review of Souces

More information

( ) Make-up Tests. From Last Time. Electric Field Flux. o The Electric Field Flux through a bit of area is

( ) Make-up Tests. From Last Time. Electric Field Flux. o The Electric Field Flux through a bit of area is Mon., 3/23 Wed., 3/25 Thus., 3/26 Fi., 3/27 Mon., 3/30 Tues., 3/31 21.4-6 Using Gauss s & nto to Ampee s 21.7-9 Maxwell s, Gauss s, and Ampee s Quiz Ch 21, Lab 9 Ampee s Law (wite up) 22.1-2,10 nto to

More information

A moving charged particle creates a magnetic field vector at every point in space except at its position.

A moving charged particle creates a magnetic field vector at every point in space except at its position. 1 Pat 3: Magnetic Foce 3.1: Magnetic Foce & Field A. Chaged Paticles A moving chaged paticle ceates a magnetic field vecto at evey point in space ecept at its position. Symbol fo Magnetic Field mks units

More information

Chapter Sixteen: Electric Charge and Electric Fields

Chapter Sixteen: Electric Charge and Electric Fields Chapte Sixteen: Electic Chage and Electic Fields Key Tems Chage Conducto The fundamental electical popety to which the mutual attactions o epulsions between electons and potons ae attibuted. Any mateial

More information

University Physics (PHY 2326)

University Physics (PHY 2326) Chapte Univesity Physics (PHY 6) Lectue lectostatics lectic field (cont.) Conductos in electostatic euilibium The oscilloscope lectic flux and Gauss s law /6/5 Discuss a techniue intoduced by Kal F. Gauss

More information

Magnetic fields (origins) CHAPTER 27 SOURCES OF MAGNETIC FIELD. Permanent magnets. Electric currents. Magnetic field due to a moving charge.

Magnetic fields (origins) CHAPTER 27 SOURCES OF MAGNETIC FIELD. Permanent magnets. Electric currents. Magnetic field due to a moving charge. Magnetic fields (oigins) CHAPTER 27 SOURCES OF MAGNETC FELD Magnetic field due to a moving chage. Electic cuents Pemanent magnets Magnetic field due to electic cuents Staight wies Cicula coil Solenoid

More information

e = 1.60 x 10 ε 0 = 8.85 x C 2 / Nm 2 V i...) F a = m Power =

e = 1.60 x 10 ε 0 = 8.85 x C 2 / Nm 2 V i...) F a = m Power = Equations: 1 1 Constants: q q v v F = k F = qe e = 1.6 x 1-19 C q 1 q 1 9 E = k = k = = 9 1 Nm / C 4πε 4 πε Φ = E da Φ V Total v v q = E da = = V f V i = W q enclosed ε = E ds U e V = q q V V V V = k E

More information

3.8.1 Electric Potential Due to a System of Two Charges. Figure Electric dipole

3.8.1 Electric Potential Due to a System of Two Charges. Figure Electric dipole 3.8 Solved Poblems 3.8.1 Electic Potential Due to a System o Two Chages Conside a system o two chages shown in Figue 3.8.1. Figue 3.8.1 Electic dipole Find the electic potential at an abitay point on the

More information

Voltage ( = Electric Potential )

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

More information

Ch 30 - Sources of Magnetic Field! The Biot-Savart Law! = k m. r 2. Example 1! Example 2!

Ch 30 - Sources of Magnetic Field! The Biot-Savart Law! = k m. r 2. Example 1! Example 2! Ch 30 - Souces of Magnetic Field 1.) Example 1 Detemine the magnitude and diection of the magnetic field at the point O in the diagam. (Cuent flows fom top to bottom, adius of cuvatue.) Fo staight segments,

More information

Module 05: Gauss s s Law a

Module 05: Gauss s s Law a Module 05: Gauss s s Law a 1 Gauss s Law The fist Maxwell Equation! And a vey useful computational technique to find the electic field E when the souce has enough symmety. 2 Gauss s Law The Idea The total

More information

JURONG JUNIOR COLLEGE Physics Department Tutorial: Electric Fields (solutions)

JURONG JUNIOR COLLEGE Physics Department Tutorial: Electric Fields (solutions) JJ 5 H Physics (646) Electic Fields_tutsoln JURONG JUNIOR COLLEGE Physics Depatment Tutoial: Electic Fields (solutions) No Solution LO Electic field stength at a point in an electic field is defined as

More information

Kinetic energy, work, and potential energy. Work, the transfer of energy: force acting through distance: or or

Kinetic energy, work, and potential energy. Work, the transfer of energy: force acting through distance: or or ENERGETICS So fa we have been studying electic foces and fields acting on chages. This is the dynamics of electicity. But now we will tun to the enegetics of electicity, gaining new insights and new methods

More information

Hopefully Helpful Hints for Gauss s Law

Hopefully Helpful Hints for Gauss s Law Hopefully Helpful Hints fo Gauss s Law As befoe, thee ae things you need to know about Gauss s Law. In no paticula ode, they ae: a.) In the context of Gauss s Law, at a diffeential level, the electic flux

More information

DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS IB PHYSICS

DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS IB PHYSICS DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS IB PHYSICS TSOKOS LESSON 10-1 DESCRIBING FIELDS Essential Idea: Electic chages and masses each influence the space aound them and that influence can be epesented

More information

From last times. MTE1 results. Quiz 1. GAUSS LAW for any closed surface. What is the Electric Flux? How to calculate Electric Flux?

From last times. MTE1 results. Quiz 1. GAUSS LAW for any closed surface. What is the Electric Flux? How to calculate Electric Flux? om last times MTE1 esults Mean 75% = 90/120 Electic chages and foce Electic ield and was to calculate it Motion of chages in E-field Gauss Law Toda: Moe on Gauss law and conductos in electostatic equilibium

More information

Solutions. V in = ρ 0. r 2 + a r 2 + b, where a and b are constants. The potential at the center of the atom has to be finite, so a = 0. r 2 + b.

Solutions. V in = ρ 0. r 2 + a r 2 + b, where a and b are constants. The potential at the center of the atom has to be finite, so a = 0. r 2 + b. Solutions. Plum Pudding Model (a) Find the coesponding electostatic potential inside and outside the atom. Fo R The solution can be found by integating twice, 2 V in = ρ 0 ε 0. V in = ρ 0 6ε 0 2 + a 2

More information

Today s Plan. Electric Dipoles. More on Gauss Law. Comment on PDF copies of Lectures. Final iclicker roll-call

Today s Plan. Electric Dipoles. More on Gauss Law. Comment on PDF copies of Lectures. Final iclicker roll-call Today s Plan lectic Dipoles Moe on Gauss Law Comment on PDF copies of Lectues Final iclicke oll-call lectic Dipoles A positive (q) and negative chage (-q) sepaated by a small distance d. lectic dipole

More information

4. Compare the electric force holding the electron in orbit ( r = 0.53

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

More information

University of Illinois at Chicago Department of Physics. Electricity & Magnetism Qualifying Examination

University of Illinois at Chicago Department of Physics. Electricity & Magnetism Qualifying Examination E&M poblems Univesity of Illinois at Chicago Depatment of Physics Electicity & Magnetism Qualifying Examination Januay 3, 6 9. am : pm Full cedit can be achieved fom completely coect answes to 4 questions.

More information

Chapter 21: Gauss s Law

Chapter 21: Gauss s Law Chapte : Gauss s Law Gauss s law : intoduction The total electic flux though a closed suface is equal to the total (net) electic chage inside the suface divided by ε Gauss s law is equivalent to Coulomb

More information

Dynamics of Rotational Motion

Dynamics of Rotational Motion Dynamics of Rotational Motion Toque: the otational analogue of foce Toque = foce x moment am τ = l moment am = pependicula distance though which the foce acts a.k.a. leve am l l l l τ = l = sin φ = tan

More information

UNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics

UNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics UNIVERSITY OF SASKATCHEWAN Depatment of Physics and Engineeing Physics Physics 115.3 Physics and the Univese FINAL EXAMINATION Decembe 21, 2016 NAME: (Last) Please Pint (Given) Time: 3 hous STUDENT NO.:

More information

2/26/2014. Magnetism. Chapter 20 Topics. Magnets and Magnetic Fields. Magnets and Magnetic Fields. Magnets and Magnetic Fields

2/26/2014. Magnetism. Chapter 20 Topics. Magnets and Magnetic Fields. Magnets and Magnetic Fields. Magnets and Magnetic Fields Magnets and Magnetic ields Magnetism Howee, if you cut a magnet in half, you don t get a noth pole and a south pole you get two smalle magnets. ectue otes Chapte 20 Topics Magnets and Magnetic ields Magnets

More information

When a mass moves because of a force, we can define several types of problem.

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

More information

TUTORIAL 9. Static magnetic field

TUTORIAL 9. Static magnetic field TUTOIAL 9 Static magnetic field Vecto magnetic potential Null Identity % & %$ A # Fist postulation # " B such that: Vecto magnetic potential Vecto Poisson s equation The solution is: " Substitute it into

More information

Phys-272 Lecture 18. Mutual Inductance Self-Inductance R-L Circuits

Phys-272 Lecture 18. Mutual Inductance Self-Inductance R-L Circuits Phys-7 ectue 8 Mutual nductance Self-nductance - Cicuits Mutual nductance f we have a constant cuent i in coil, a constant magnetic field is ceated and this poduces a constant magnetic flux in coil. Since

More information

20-9 ELECTRIC FIELD LINES 20-9 ELECTRIC POTENTIAL. Answers to the Conceptual Questions. Chapter 20 Electricity 241

20-9 ELECTRIC FIELD LINES 20-9 ELECTRIC POTENTIAL. Answers to the Conceptual Questions. Chapter 20 Electricity 241 Chapte 0 Electicity 41 0-9 ELECTRIC IELD LINES Goals Illustate the concept of electic field lines. Content The electic field can be symbolized by lines of foce thoughout space. The electic field is stonge

More information

Physics 2020, Spring 2005 Lab 5 page 1 of 8. Lab 5. Magnetism

Physics 2020, Spring 2005 Lab 5 page 1 of 8. Lab 5. Magnetism Physics 2020, Sping 2005 Lab 5 page 1 of 8 Lab 5. Magnetism PART I: INTRODUCTION TO MAGNETS This week we will begin wok with magnets and the foces that they poduce. By now you ae an expet on setting up

More information

Target Boards, JEE Main & Advanced (IIT), NEET Physics Gauss Law. H. O. D. Physics, Concept Bokaro Centre P. K. Bharti

Target Boards, JEE Main & Advanced (IIT), NEET Physics Gauss Law. H. O. D. Physics, Concept Bokaro Centre P. K. Bharti Page 1 CONCPT: JB-, Nea Jitenda Cinema, City Cente, Bokao www.vidyadishti.og Gauss Law Autho: Panjal K. Bhati (IIT Khaagpu) Mb: 74884484 Taget Boads, J Main & Advanced (IIT), NT 15 Physics Gauss Law Autho:

More information

2 E. on each of these two surfaces. r r r r. Q E E ε. 2 2 Qencl encl right left 0

2 E. on each of these two surfaces. r r r r. Q E E ε. 2 2 Qencl encl right left 0 Ch : 4, 9,, 9,,, 4, 9,, 4, 8 4 (a) Fom the diagam in the textbook, we see that the flux outwad though the hemispheical suface is the same as the flux inwad though the cicula suface base of the hemisphee

More information

Module 12: Current and Resistance 1

Module 12: Current and Resistance 1 Module 12: Cuent and Resistance 1 Table of Contents 6.1 Electic Cuent... 6-2 6.1.1 Cuent Density... 6-2 6.2 Ohm s Law... 6-4 6.3 Electical Enegy and Powe... 6-7 6.4 Summay... 6-8 6.5 Solved Poblems...

More information

OSCILLATIONS AND GRAVITATION

OSCILLATIONS 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 information