DEPARTMENT OF ELECTRICAL AND ELECTRONICS ENGINEERING
|
|
- Lesley Jenkins
- 5 years ago
- Views:
Transcription
1 DEPARTMENT OF ELECTRICAL AND ELECTRONICS ENGINEERING EE 630 ELECTROMAGNETIC THEORY UNIT-I ELECTROSTATICS I PART A. Mention an two souces of electomagnetic fields (o) What ae the souces of vaious tpes of EMF? Cuent caing conductos. Mobile phones. Micowave oven. Compute and Television sceen. High voltage Powe lines.. How can a vecto field be epessed as the gadient of a scala field? The gadient of an scala function is the maimum space ate of change of that function. If the scala V epesents electic potential, V epesents potential gadient. This opeation is called the gadient. Gadient of a scala is a vecto. 3. What is the phsical significance of the tem divegence of a vecto field? The divegence of the vecto field is the outflow fom a small closed suface pe unit volume as the volume shinks to zeo. 4. Define cul of a vecto. The cul of a vecto A at an point is defined as the limit of its suface integal of its coss poduct with nomal ove a closed suface pe unit volume as the volume shinks to zeo. A Cul A 5. Show that the vectos A and B ae paallel A = a + 4a + a z ; B = 4a + 8a +a z. Theefoe vectos A and B ae paallel to each othe. 6. Pove that cul gad Ф = 0 a a z a A B 4 = [8-8] [4-4] + [6-6] = 0 a 4 z a 8 a z a a a z z
2 Thus poved = ( ) a z z = 0 ( ) a z z ( ) az 7. How the unit vectos ae defined in clindical Co-odinate sstems? Unit vectos is having unit magnitude and diected along the co-odinates aes. Fo clindical Co-odinate Whee 8. Given A (Ma/June 009) a A a A a Z Az a, a & a z, ae unit vectos in the diection of,, z espectivel. A 0a 3a z and B5a 4a find the angle (o) pojection of A and B The angle Ө AB can be found b eithe dot o coss poduct A. B = (0, 0, 3). (5, 4, 0) = 40 A B 4 4 COS Ө AB = A. B A. B = Ө AB = Calculate the total chage within the volume of the univese, if v e 3 c m Fo Sphee dv = sinө d dө dф Total chage Q = v Vol e 0 dv = d sin d d 0 0
3 Q =.73π coulomb 0. What ae the tpes of co-odinate sstems? Catesian (o) ectangula co- odinate sstem Clindical co- odinate sstem Spheical co- odinate sstem. What is the diffeence between scala and vecto quantit? S.No. Scala Vecto. It is a quantit which is completel chaacteized b its magnitude. It is a quantit which is completel chaacteized b its magnitude and diection.. Eample: mass, volume, densit. Eample: foce, velocit, displacement.. Given the two coplana vecto A=3a +4a -5a z ; B=-6a +a +4a z ; Obtain the unit vecto nomal to the plane of the vectos A and B. AB = B A = (6-3)a + (-4)a + (4+5)a z AB = -9a -a +9a z AB =.88 Unit vecto = AB AB = a a a z 3. Convet the given point A(,, 3 ) in spheical co-odinates into Catesian co-odinates Given = Tansfom = sinө cosф = sin ( ) cos ( 3 ) Ө = = = sinө sinф = sin ( ) sin ( 3 ) Ф = 3 =.00 z = cosө = cos ( ) =.99
4 Catesian co-odinates ae (0.055,.00,.99). 4. State divegence theoem. The integal of the nomal component of an vecto field ove a closed suface is equal to the integal of the divegence of this vecto field ove a volume enclosed b the closed suface. 5. State stoke s theoem. The line integal of a vecto aound a closed path is equal to the suface integal of the nomal component of its cul ove an suface bounded b the path. 6. Epess the value of diffeential length, suface in ectangula co-odinate sstem. d d dz The diffeential length dl = The diffeential aea ds = d d = d dz = dz d 7. Epess the Gadient of a vecto in the thee sstem of othogonal co-odination. Fo Catesian coodinates sstem Fo clindical coodinates sstem Fo spheical coodinates sstem 8. Show that the two vectos A 6a a 5a and B 3( a a a ) each othe. z z ae pependicula to A. B = (6 3) + ( (-3)) + ((-5) ) = 0
5 9. Find the gadient of the scala field, A = Z COS A A A. A a a az z = ( z cos ) a ( z cos ) a ( z cos ) az z 0. Define vecto field. A = z[sin cos ] cos If a quantit which is specified in a egion to design a field is a vecto, then the coesponding field is called vecto field. E: The velocit of paticles in a moving fluid, wind velocit of atmosphee, displacement of a fling bid in a space.. State Gauss s Law The electic flu passing though an closed suface is equal to the total chage enclosed b that suface Q PART B. What ae the diffeent co-odinate sstems used to epesent field vectos? Discuss about them in bief.. Find the gadient of the following scala fields: (i) V = e -z sin cosh (ii) U = Z COS (iii) W = 0 sin θ cosф 3. Detemine the divegence of these vecto fields: (i) P = z a + z a z (ii) Q = sin a za z a cos z (iii) T = cos a sin cos a cos a 4. State and Eplain Divegence and Stoke s theoems 5. Given A cos I I in clindical co-odinate. Fo the contou shown veif Stoke s theoem. 6. Given points P(-,6,3) and vecto A=a +(+z)a, epess P and A in clindical and spheical coodinates. Evaluate A at P in the Catesian, clindical and spheical sstems.
6 7. Check validit of the divegence theoem consideing the field D= a+ a c/m and the ectangula paallelepiped fomed b the planes =0,=,=0,= &z=0,z=3 8. Veif the divegence theoem fo the following case A=XY a +Y 3 a +Y Za z and the suface is a cuboid defined b 0<<, 0<< & 0<z< 9. Given that F= X Ya -Ya. find F. dl whee L is shown in fig. & also veif the stoke s theoem. 0.Dive an epession fo the electic field due to a staight and infinite Unifoml chaged wie of length L metes and with a chage densit of +λ c/m at a point P which lies along the pependicula bisecto of wie.. Using Gauss s law calculate the E due to infinitel lage unifoml chaged plate.. Find the Electic potential at a point (4,3)m due to a chage of 0-9 clo at the oigin in fee space. 3. Thee point chages Q =0-6 c,q =-0-6 c and Q 3 = c ae located in ai (fee space) at the cones of an equilateal tiangle of 50cm side. Detemine the magnitude and diection of the foce on Q 3, Also find Electic field at Q ( i) A cicula disc of adius a, m is chaged unifoml with a chage densit of σ C/m Find the electic field intensit at a point h, m fom the disc along its ais. (ii) A cicula disc of 0 cm adius is chaged unifoml with a total chage of 0-6 c. Find the electic intensit at a point 30 cm awa fom the disc along the ais.
7 EE 630 ELECTROMAGNETIC THEORY UNIT-II ELECTROSTATICS II PART A. Define Electic field intensit o Electic field. The electic field intensit o the electic field stength at a point is defined as the foce pe unit chage. That is. What is the pactical significance of dielectic stength? The minimum value of the applied electic field at which the dielectic beakdown occus is Called dielectic stength. 3. What is an Electic dipole? Dipole o Electic dipole is nothing but two equal and opposite point chages ae sepaated b a ve small distance. 4. Define polaization Polaization is defined as dipole moment pe unit volume 5. State Coulomb s Law The foce between two pat chages is popotional to the poduct of chages and is invesel popotional to the squae of distance between them. 6. Wite down the epessions fo Laplace s and Poisson s equations Poisson s equations : Laplace s equations
8 7. State the vecto fom of electic flu densit The electic flu densit is defined as electic flu pe unit aea. It is denoted b D D=Q/A (c/m) the flu densit vecto is defined as: 8. Wite the capacitance in a coaial cable? C 0 ln( b / a) F/m 9. A unifom line chage with P L = 5 c / m lies along the -ais. Find E at (3,,)m. Given data: P L = 5 c / m Find: Fomula: E (Electic field intensit) =? E l 0 = (3,,)m E = (V/m) What is the significance phsical diffeence between Poisson s and Laplace s equation? Poisson s and Laplace equation ae useful fo detemining the electostatic potential V in egions at whose boundaies ae known. When the egion of inteest contains chages in a known distibution v can be used to detemine the potential function. Poisson s equation. The electical potential nea the oigin of a sstem of co-odinates is V=a +b +cz.find the field at (,4,6). Given data: V=a +b +cz (,,z) = (,4,6) Find : Field (E) =? Fomula: E = V E = V = V a V a V a z V = ( a a b a cz a ) At (,4,6) E = (a a 4b a 6c a ) V/m. z z z a a b a cz az
9 . Wite the poisson s & laplace's equations. Poisson s equation: Whee V - V V is the potential is the volume chage densit v is the dielectic constant o pemittivit of the medium. Laplace's equations: V 0 3. Wite down the magnetic bounda conditions. i) The nomal components of flu densit B ae continuous acoss the bounda. ii) The tangential components of field intensit H is continuous acoss the bounda 4. Define potential Potential at an point is defined as the wokdone is moving a unit positive chage fom infinit to that point in an electic field. Q V 4 5. Define capacitance It is defined as the atio of magnitude of chage on eithe of the conducto to the potential diffeence between conductos. It is given b Q C V 6. Descibe what ae the souces of electic field and magnetic fields. Stationa chages poduce electic field that ae constant in time: hence the tem electostatics. Moving chages (stead cuents) poduce magnetic fields that ae constant in time; hence the tem magnetostatics.
10 7. If V [ 0 Given data: find E and D V 0 Find : E & D =? Fomula: E = V D E V V V V = a a az z E = - 0 [ ( ) ( ) ( ) ] z = 40 ] ) ) ( ( D = 40 [ ] ) ) ( ( 8. Name a few applications of Gauss s Law in electostatics. Gauss s Law is applied to detemine the electic field intensit fom a closed suface.(e.g) Electic field can be detemine fo shell, two concentic shell o clindes, etc. 0. What is the use of Gauss s Law? Gauss s law is paticulal useful in detemining the electic field E of a chage distibution with some smmet condition. PART B ) (a) A total chage of 0-8 C is distibuted unifoml along a ing of adius of 5m. Calculated the potential on the ais of the ing at a point 5m fom the cente of the ing. (b) Conducting spheical shells with adii a=0cm and b=30cm ae maintained at a potential diffeence of 00V such that V (=b) = 0 and V (=b) = 00 volts. Detemine V and E in the egion between the shells. ) (a) Point chages mc and -mc ae located at (3,,-) and (-,-,-4) espectivel. Calculate the electic foce on a 0Nc chage located at (0,3,) and the electic field intensit at that point. (b) A dielectic sphee ( 5. 7 ) of adius 0cm has a point chage PC placed at its cente. Calculate: (i) The suface densit of polaization chage on the suface of the sphee (ii) The foce eeted b the chage on a -4 Pc point chage placed on the sphee.
11 3) (a) Deive the bounda conditions at the chage inteface of two dielectic media. (b) State and pove Gauss s Law 4) Discuss Electic field in fee space, dielectic and in conductos. 5) Conducting spheical shells with adii a=0cm and b=30cm ae maintained at a potential diffeence of 00v such that V(=b)=0 and V(=a)=00volts. Detemine v and E in the ejoin between the shells. 6) Detemine the capacitance of a capacito consisting of two paallel metal plates 30cm 30cm suface aea sepaated b 5mm in ai. What is the total eneg stoed b the capacito if the capacito is chaged to a potential diffeence of 500v? 7) What is dipole moment? Obtain epession fo the potential and field due to an electic dipole.two point chages Q = 4nC, Q = nc ae kept at (, 0, 0) and (6, 0, 0). Epess the electic field at (4, -, ) 8. Deive epession fo potential due to a dipole. 9. Deive epession fo eneg and eneg densit in a electic field. 0. Deive an epession fo capacitance between two paallel wies.. Deive the electic bounda conditions.
12 EE 630 ELECTROMAGNETIC THEORY UNIT-III MAGNETOSTATICS PART A. State Biot Savat law. It states that the magnetic flu densit at an point due to cuent element is popotional to the cuent element and sine of the angle between the element length and line joining and invesel popotional to the squae of the distance between them. I dl 0 db sin 4. State Ampee s cicuital law Magnetic field intensit aound a closed path is equal to the cuent enclosed b the path. H.dl I 3. Define the tem Magnetization. Magnetisation is defined as the atio of magnetic dipole moment to unit volume. A M Q a ( ) M Volume m A 4. What do ou mean b magnetic moment? A small ba magnet of length l with pole stength Qm ma be consideed as magnetic dipole. The poduct of pole stength Qm and length l is called magnetic moment. m = Q m l Magnetic dipole is consideed as equivalent to cuent loop with aea A and caing a cuent I. The magnetic moment is, m = I A 5. Give fou similaities between Electostatic field magnetic field. Sl.No. Electo Static field Magnetic field Eneg stoed is ½ CV Eneg stoed is ½ LI Chages ae at est Chages ae at motion 3 Electic flu densit E V/m Magnetic flu densit H A/m 4 Electic flu densit D = E C/m Magnetic flu densit B = H Wb/m 6. What is H due to a long staight cuent caing conducto. The Magnetic field intensit at an point due to long staight conducto of caing cuent of I with a distance of d is I H d 7. Distinguish between magnetic scala potential and magnetic vecto potential. Sl.No. Magnetic scala potential Magnetic vecto potential It is defined as dead quantit whose negative gadient gives the magnetic intensit if thee is no cuent souce pesent. It is defined as that quantit whose cul gives the magnetic flu densit H BA Vm m
13 8. State Loent s Law and application If a chage paticle is moving with velocit v in the pesence of both an electic field E and a magnetic field B, then the total electomagnetic foce acting on it is F Q( E v B) This is called Loentz foce. Applications: i. Used to detemine electon o bits in magneton. ii. Used to detemine poton path in ccloton. iii. iv. Used to detemining plasma chaacteistics in a magneto hdodnamic geneato. Used to detemine the motion of chaged paticle in a combined electic and magnetic field. 9. A long staight wie caies a cuent I= Amp. At what distance is the magnetic field H= A/m. Given data: I = Amp H= A/m. Find : d =? Fomula: I I H = d = d H d = = 0.59 Result: d = 0.59 m 0. Detemine the foce pe unit length between two long paallel wies sepaated b 5cm in ai and caing cuents of 40A in the same diection. Given data: Find : Fomula: Result: I = I = 40 A d= A/m. Foce/length =? Foce/length = I 0 I d Foce/length = - 5 Foce/length = N/m = Define self inductance. The self inductance of a coil is defined as the ate of total magnetic flu linkage to the cicuit though the coil. L N i Whee, --- Magnetic flu N --- No. of tuns of coil I --- Cuent
14 . Define mutual inductance. The mutual inductance between two coils is defined as the ate of induced magnetic flu linkage in one coil to the though in othe coil. M N i Whee, N ---- No.of tuns in coil magnetic flu links coil i ---- cuent though coil 3. Compae the eneg stoed in inducto and capacito. Fo magnetic field, Eneg stoed in inducto W = ½ LI Fo electic field, Eneg stoed in capacito W = ½ CV 4. A egion in fee space has a magnetic field intensit of B web/m. What is the eneg stoed pe m 3 of space? Eneg densit = eneg pe volume = ½ B Joules/m 3 Whee, ---- is the pemeabilit of the medium. B ---- magnetic field intensit 5. Calculated the emf induced in a cicuit in a cicuit having an inductance of 700 H cuent though it vaies at a ate of 5000 A pe second. Given data: L = 700 H if the Find : Fomula: Result: di 5000 A/ s dt Induced emf ( v ) =? v L di dt v = v = 3.5 volts. 6. What will be the magnetic field of a tooidal solenoid ( with N tuns, caing a cuent I) within the volume of the ing and outside the ing? magnetic field intensit of a tooidal solenoid is given b N I H (inside ing) H = 0 (outside ing) 7. What is the significance of eneg densit? It depends on what factos? It indicates the amount of eneg stoed/unit volume of a sstem (electic o magnetic). Moe is the eneg densit moe will be the wok done fo the given volume. It depends on the medium fo the given field (Electic E o Magnetic H)
15 8. What is solenoid? An inducto coil consisting of multiple tuns of wie wound in a helical geomet aound a clindical coe is called as solenoid. 9.Give the epession fo inductance of a solenoid. N A 0 L l Whee, N -- is numbe of tuns. A -- is aea of coss-section. l -- is length of solenoid. --is fee space 0 pemeabilit 0. Distinguish between solenoid and tooid. Solenoid is a clindicall shaped coil consisting of a lage numbe of closel spaced tuns of insulated wie wound usuall on a non-magnetic fame. If a long, slende solenoid is bent into the fom of a ing and theeb closed on itself, it becomes tooid.. PART B a) An Ion ing with a coss sectional aea of 3cm and a mean cicumfeence of 5cm is wound with 50 tuns of wie caing a cuent of 0.3A. The elative pemeabilit of the ing is 500. Calculate the flu established in the ing. b) Region, 0 z m is occupied b an infinite slab of pemeable mateial(. 5 ).If B = 0a 5a m wb/m within the slab, detemine: i. J ii. J b iii. M iv. K b on z=0. a) The -plane seves as the inteface between two diffeent media. Medium (z < 0) is filled with a mateial whose 6, and medium (z > 0) is filled with a mateial whose 4. If the inteface caies cuent a m A/m, and B = 5a + 8a z m wb/m, find H and B o b) A small cuent loop L with magnetic moment 5a z A.m is located at the oigin while anothe small loop cuent L with magnetic moment 3a A.m is located at (4,-3,0). Detemine the toque on L a) Establish the elation of foce between cuent caing paallel conductos. b) Obtain the magnetic flu densit on the ais of a cicula coil caing cuent I. a) Deive an epession fo inductance of a solenoid with N tuns and l mete length caing of I ampees. b) Deduce the epession to find the magnetic field intensit H at an point P due to an infinite filamentat cuent caing conducto lies in Z-ais and caing I ampee. a) State and Eplain Ampee s cicuital law, Biot Savat law. b) State and Eplain Loent s Law
16 EE 630 ELECTROMAGNETIC THEORY UNIT-IV ELECTRODYNAMIC FIELDS PART A. State Faada s law of induction.. State lenz s law 3. Give the equation of tansfome emf 4. What is motional electic field? 5. What is motinal emf? 6. What is the emf poduced b moving loop in time vaing field? 7. What is time hamonic field? 8. Give time hamonic mawell s equation in point fom. assume time facto e -jωt 9. Distingush between Field theo and Cicuit theo 0. Wite Mawell s equation in point and integal fom fo good conductos.. What Is significance of displacement cuent densit?. In a mateial fo which σ= 5s/m and ξ= and E=50 sin 0 0t (V/m) find the conduction and displacement cuent densities. PART- B. What ae the diffeent was of EMF geneation? Eplain with the govening equations and suitable pactical eamples. (6). With necessa eplanation, deive the Mawell s equation in diffeential and integal foms (6) 3. What do ou mean b displacement cuent? wite down the epession fo the total cuent densit (8) 4.(a) Find the total cuent in a cicula conducto of adius 4mm if the cuent densit vaies accoding to J=0 4 /R A/m. (8) (b) Given the conduction cuent densit in a loss dielectic as Jc=0.0 sin 0 9 t A/m.find the displacement cuent densit if σ=0 3 mho/m and ξ=6.5 (8) 5 (a) Eplain the elation between field theo and cicuit theo. (8) (b)the magnetic field intensit in fee space is given as H=H 0 sinθa t A/m. whee θ=ωt-βz and β is a constant quantit. Detemine the displacement cuent densit. (8) 6 (a) Wite shot notes on faadas law of electomagnetic induction. (8) (b) Show that the atio of the amplitudes of the conduction cuent densit and displacement cuent densit is σ/ωξ, fo the applied field amplitude atio if the applied field is E=Em e -t/λ whee λ is eal. (8) 7. Deive Geneal field elation fo time vaing electic and magnetic fields using Mawell s equations. (6)
17 EE 630 ELECTROMAGNETIC THEORY UNIT-V ELECTROMAGNETIC WAVES PART A. What is wave? If a phsical phenomenon that occus at one place at a given time is epoduced at othe places at late times, the time dela being popotional to the space sepaation fom the fist location, then the goup of phenomena constitute a wave.. Give the wave equation in tems of electic field and magnetic field. The electomagnetic wave equation in tems of electic field is, E E E 0 t t The electomagnetic wave equation in tems of magnetic field is, H H H 0 t t 3. Give the wave equation in fee space. E t H t The wave equation in fee space in tems of electic field is, E 0 The wave equation in fee space in tems of magnetic field is, H 0 4. List out the popeties of a unifom plane wave. If the plane of wave is the same fo all points on a plane suface, it is called plane wave. If the amplitude is also constant in a plane wave, it is called unifom plane wave. The popeties of unifom plane waves ae: a) At eve point in space, E and H ae pependicula to each othe and to the diection of tavel. b) The fields va with time at the same fequenc, evewhee in space. c) Each field has the same diection, magnitudes and phase at eve point in an plane pependicula to the diection of wave tavel. 5. Give the epession fo the chaacteistic impedance of the wave. The chaacteistic impedance o intinsic impedance is the atio of the electic field intensit to the magnetic field intensit. E H of the medium. whee, 6. What is Vecto Helmholtz equation. is the pemeabilit of the medium and ε is the pemittivit The wave equation in lossless medium in phaso fom is called the vecto Helmholtz equation. E E 0 7. Give the wave equation fo a conducting medium. The wave equation fo a conducting medium in phaso fom is given as, E j j ) E 0
18 8. What is skin effect and skin depth? In a good conducto the wave is attenuated as it pogesses. At highe fequencies the ate of attenuation is ve lage, and the wave ma penetate onl a ve shot distance befoe being educed to a small value. This effect is called skin effect. The skin depth () is defined as that depth in which the wave has been attenuated to /e o appoimatel 37% of its oiginal value. It is also known as depth of penetation. whee, is the attenuation constant, 9. Give the epession fo attenuation constant and phase shift constant fo a wave popagating in a conducting medium. The attenuation constant fo a wave popagating in a conducting medium is, The phase shift constant fo a wave popagating in a conducting medium is, 0. Give the epession fo the velocit of popagation of a wave in an medium. The velocit of popagation of a wave in an medium is v whee, is the angula velocit and is the phase shift.. Define pointing theoem. The vecto poduct of electic field intensit and magnetic field intensit at an point is a measue of the ate of eneg flow pe unit aea at that point. P E H. What is Bewste angle? Bewste angle is an incident angle at which thee is no eflected wave fo paallel polaized wave. tan Whee is dielectic constant of medium is dielectic constant of medium 3. State one dimensional wave equation. E t E
19 4. What is the velocit of electomagnetic wave in fee space and in lossless dielectic. v 0 0 c m/s 5. Repesent equation of electomagnetic wave in the phaso fom. Wave equation in phaso fom is E E j E 0 O E E 0 Whee j ( j ) 6. Fo a loss dielectic mateial having, 48, 0s / m. Calculate the popagation constant at a fequenc of 6GHZ. Given data: 48 0s / m. f = 6MHZ Find: popagation constant ( ) Fomula: j( j ) Soluation:.3 j ( j ) j ( j.3) = j 5668 = = Result: = Bief about the intinsic impedance fo a pefect dielectic medium. Intinsic impedance fo a pefect dielectic medium is given b j je E Ω is a eal positive, Phase angle is zeo, Fo a pefect dielectic, both the field E and H ae in phase. 8. Bief about comple pointing vecto. The comple pointing vecto is given b P = ½ E H Poduct of E and H is a vecto poduct. Mutuall pependicula components of E and H contibute to the powe flow. This powe flow is diected along the nomal to the plane containing E and H.
20 9. What is mean b Linea polaization? The electic field E is the esultant of E X and E Y, and the diection of it depends on the elative magnitude of E X and E Y. The angle made b E with ais is given b tan E E If the esultant E is oiented in a diection which is constant with time, the wave is said to be lineal polaized. 0. State Snell s Law. When a wave is tavelling fom one medium to anothe medium, the angle of incidence is elated to angle of eflection as follows. sin sin i t PART B. a) A plane wave popagating though a medium with = 8, = has z / 3 8 E 0.5e sin ( 0 t z) a. V / m. and H field. Detemine, Wave velocit, The loss tangent, intinsic impedance b) deive the geneal electomagnetic wave equation.. a) Fo a paallel polaized wave, eplain cleal about Snell s Law and citical angle. b) Sea wate plas a vital ole in the stud of submaine communications. Assuming that fo seawate = 4 S/m, = 80, = and f= 00 MHz.Calculate a) The phase velocit b) The wavelength c) The skin depth d) The intinsic impedance a)an electic field in fee space is given b E 50cos ( t ). V /. Find the diection of the wave popagation, calculate phase constant and the time taken to tavel a distance of /. b) Pove pointing theoem a 0 m 4. a)a loss mateial has = 5, =. If at 5MHZ,the phase constant is 0 ed/m. calculate the loss tangent, the pemittivit, the attenuation constant and the intinsic impedance. b) Fo a paallel polaized wave, eplain cleal about Snell s Law and citical angle. 5. a) Eplain the wave popagation in loss dielectics. b) Define the tems: intinsic impedence, popagation constant, election and efaction coefficients.
EC6403 Electromagnetic Fields Department of ECE COURSE OUTCOMES. Divergence
EC6403 Electomagnetic Fields Depatment of ECE 017-018 COURSE OUTCOMES UNIT I : Static Electic field PART A - C1.1 1. Define scala and vecto quantities. Scala quantit: A scala is a quantit which is completel
More informationReview: Electrostatics and Magnetostatics
Review: Electostatics and Magnetostatics In the static egime, electomagnetic quantities do not vay as a function of time. We have two main cases: ELECTROSTATICS The electic chages do not change postion
More informationTUTORIAL 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 informationPhysics 122, Fall October 2012
hsics 1, Fall 1 3 Octobe 1 Toda in hsics 1: finding Foce between paallel cuents Eample calculations of fom the iot- Savat field law Ampèe s Law Eample calculations of fom Ampèe s law Unifom cuents in conductos?
More information4. Electrodynamic fields
4. Electodynamic fields D. Rakhesh Singh Kshetimayum 1 4.1 Intoduction Electodynamics Faaday s law Maxwell s equations Wave equations Lenz s law Integal fom Diffeential fom Phaso fom Bounday conditions
More informationFields and Waves I Spring 2005 Homework 8. Due: 3 May 2005
Fields and Waves I Sping 005 Homewok 8 Tansmission Lines Due: 3 May 005. Multiple Choice (6) a) The SWR (standing wave atio): a) is a measue of the match between the souce impedance and line impedance
More information2. Electrostatics. Dr. Rakhesh Singh Kshetrimayum 8/11/ Electromagnetic Field Theory by R. S. Kshetrimayum
2. Electostatics D. Rakhesh Singh Kshetimayum 1 2.1 Intoduction In this chapte, we will study how to find the electostatic fields fo vaious cases? fo symmetic known chage distibution fo un-symmetic known
More informationMAGNETIC 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 informationElectrostatics (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 informationPhys-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 informationEM-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 informationA 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 information3. Magnetostatic fields
3. Magnetostatic fields D. Rakhesh Singh Kshetimayum 1 Electomagnetic Field Theoy by R. S. Kshetimayum 3.1 Intoduction to electic cuents Electic cuents Ohm s law Kichoff s law Joule s law Bounday conditions
More informationCh 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 informationF Q E v B MAGNETOSTATICS. Creation of magnetic field B. Effect of B on a moving charge. On moving charges only. Stationary and moving charges
MAGNETOSTATICS Ceation of magnetic field. Effect of on a moving chage. Take the second case: F Q v mag On moving chages only F QE v Stationay and moving chages dw F dl Analysis on F mag : mag mag Qv. vdt
More informationF = 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 informationCHAPTER 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 informationConventional Paper-I (a) Explain the concept of gradient. Determine the gradient of the given field: ( )
EE-Conventional Pape-I IES-013 www.gatefoum.com Conventional Pape-I-013 1. (a) Eplain the concept of gadient. Detemine the gadient of the given field: V ρzsin φ+ z cos φ+ρ What is polaization? In a dielectic
More informationPHYS 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( ) ( )( ) ˆ. Homework #8. Chapter 27 Magnetic Fields II.
Homewok #8. hapte 7 Magnetic ields. 6 Eplain how ou would modif Gauss s law if scientists discoveed that single, isolated magnetic poles actuall eisted. Detemine the oncept Gauss law fo magnetism now eads
More information( ) 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 informationMCV4U Final Exam Review. 1. Consider the function f (x) Find: f) lim. a) lim. c) lim. d) lim. 3. Consider the function: 4. Evaluate. lim. 5. Evaluate.
MCVU Final Eam Review Answe (o Solution) Pactice Questions Conside the function f () defined b the following gaph Find a) f ( ) c) f ( ) f ( ) d) f ( ) Evaluate the following its a) ( ) c) sin d) π / π
More informationUnit 7: Sources of magnetic field
Unit 7: Souces of magnetic field Oested s expeiment. iot and Savat s law. Magnetic field ceated by a cicula loop Ampèe s law (A.L.). Applications of A.L. Magnetic field ceated by a: Staight cuent-caying
More informationELECTROSTATICS::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 informationSEE LAST PAGE FOR SOME POTENTIALLY USEFUL FORMULAE AND CONSTANTS
Cicle instucto: Moow o Yethiaj Name: MEMORIL UNIVERSITY OF NEWFOUNDLND DEPRTMENT OF PHYSICS ND PHYSICL OCENOGRPHY Final Eam Phsics 5 Winte 3:-5: pil, INSTRUCTIONS:. Do all SIX (6) questions in section
More informationMagnetic 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 information16.1 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 information3. Electromagnetic Waves II
Lectue 3 - Electomagnetic Waves II 9 3. Electomagnetic Waves II Last time, we discussed the following. 1. The popagation of an EM wave though a macoscopic media: We discussed how the wave inteacts with
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 informationPhys102 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 informationFI 2201 Electromagnetism
FI 2201 Electomagnetism Alexande A. Iskanda, Ph.D. Physics of Magnetism and Photonics Reseach Goup Electodynamics ELETROMOTIVE FORE AND FARADAY S LAW 1 Ohm s Law To make a cuent flow, we have to push the
More informationCHAPTER 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 information11) A thin, uniform rod of mass M is supported by two vertical strings, as shown below.
Fall 2007 Qualifie Pat II 12 minute questions 11) A thin, unifom od of mass M is suppoted by two vetical stings, as shown below. Find the tension in the emaining sting immediately afte one of the stings
More informationForce 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 informationMagnetic 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 information17.1 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 informationHow Electric Currents Interact with Magnetic Fields
How Electic Cuents nteact with Magnetic Fields 1 Oested and Long Wies wote these notes to help ou with vaious diectional ules, and the equivalence between the magnetism of magnets and the magnets of electic
More informationPY208 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 informationLecture 2 Date:
Lectue 2 Date: 5.1.217 Definition of Some TL Paametes Examples of Tansmission Lines Tansmission Lines (contd.) Fo a lossless tansmission line the second ode diffeential equation fo phasos ae: LC 2 d I
More informationMagnetic Field of a Wire
Magnetic Field of a Wie Fundamental Laws fo Calculating B-field Biot-Savat Law (long method, but woks always) Ampee s Law (high symmety) B-Field of a Staight Wie Fo a thin staight conducto caying cuent
More informationEELE 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 informationPHYS 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 informationSection 1: Main results of Electrostatics and Magnetostatics. Electrostatics
Chage density ection 1: ain esults of Electostatics and agnetostatics Electostatics The most fundamental quantity of electostatics is electic chage. Chage comes in two vaieties, which ae called positive
More informationUniversity 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 informationSolutions. 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 informationPrerna Tower, Road No 2, Contractors Area, Bistupur, Jamshedpur , Tel (0657) , PART I PHYSICS
ena Towe, oad No, Contactos Aea, Bistupu, Jamshedpu 8311, Tel (657)189, www.penaclasses.com IIT JEE 1 hsics ape II AT I HYSICS SECTION I : Single Coect Answe Tpe This Section contains 8 multiple choice
More informationFaraday s Law (continued)
Faaday s Law (continued) What causes cuent to flow in wie? Answe: an field in the wie. A changing magnetic flux not only causes an MF aound a loop but an induced electic field. Can wite Faaday s Law: ε
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 informationGauss s Law: Circuits
Gauss s Law: Cicuits Can we have excess chage inside in steady state? E suface nˆ A q inside E nˆ A E nˆ A left _ suface ight _ suface q inside 1 Gauss s Law: Junction Between two Wies n 2
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 informationPhysics 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 informationIX INDUCTANCE AND MAGNETIC FIELDS
IX INDUCTNCE ND MGNETIC FIELDS 9. Field in a solenoid vaying cuent in a conducto will poduce a vaying magnetic field. nd this vaying magnetic field then has the capability of inducing an EMF o voltage
More informationUniversity 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 informationCalculate 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 informationChapter 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 informationr r q Coulomb s law: F =. Electric field created by a charge q: E = = enclosed Gauss s law (electric flux through a closed surface): E ds σ ε0
Q E ds = enclosed ε S 0 08 Fomulae Sheet 1 q 1q q Coulomb s law: F =. Electic field ceated by a chage q: E = 4πε 4πε Pemittivity of fee space: 0 1 = 9 10 4πε 0 9 Newton mete / coulomb = 9 10 9 0 N m Q
More informationSAMPLE 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 informationReview Notes on Maxwell's Equations
ELEC344 Micowave Engineeing, Sping 2002 Handout #1 Kevin Chen Review Notes on Maxwell's Equations Review of Vecto Poducts and the Opeato The del, gad o nabla opeato is a vecto, and can be pat of a scala
More informationMagnetostatics. Magnetic Forces. = qu. Biot-Savart Law H = Gauss s Law for Magnetism. Ampere s Law. Magnetic Properties of Materials. Inductance M.
Magnetic Foces Biot-Savat Law Gauss s Law fo Magnetism Ampee s Law Magnetic Popeties of Mateials nductance F m qu d B d R 4 R B B µ 0 J Magnetostatics M. Magnetic Foces The electic field E at a point in
More informationME 210 Applied Mathematics for Mechanical Engineers
Tangent and Ac Length of a Cuve The tangent to a cuve C at a point A on it is defined as the limiting position of the staight line L though A and B, as B appoaches A along the cuve as illustated in the
More informationMagnetic Fields Due to Currents
PH -C Fall 1 Magnetic Fields Due to Cuents Lectue 14 Chapte 9 (Halliday/esnick/Walke, Fundamentals of Physics 8 th edition) 1 Chapte 9 Magnetic Fields Due to Cuents In this chapte we will exploe the elationship
More informationB da = 0. Q E da = ε. E da = E dv
lectomagnetic Theo Pof Ruiz, UNC Asheville, doctophs on YouTube Chapte Notes The Maxwell quations in Diffeential Fom 1 The Maxwell quations in Diffeential Fom We will now tansfom the integal fom of the
More informationFlux. 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 informationHopefully 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 informationEM Boundary Value Problems
EM Bounday Value Poblems 10/ 9 11/ By Ilekta chistidi & Lee, Seung-Hyun A. Geneal Desciption : Maxwell Equations & Loentz Foce We want to find the equations of motion of chaged paticles. The way to do
More informationWelcome to Physics 272
Welcome to Physics 7 Bob Mose mose@phys.hawaii.edu http://www.phys.hawaii.edu/~mose/physics7.html To do: Sign into Masteing Physics phys-7 webpage Registe i-clickes (you i-clicke ID to you name on class-list)
More informationFaraday s Law. Faraday s Law. Faraday s Experiments. Faraday s Experiments. Magnetic Flux. Chapter 31. Law of Induction (emf( emf) Faraday s Law
Faaday s Law Faaday s Epeiments Chapte 3 Law of nduction (emf( emf) Faaday s Law Magnetic Flu Lenz s Law Geneatos nduced Electic fields Michael Faaday discoeed induction in 83 Moing the magnet induces
More informationDEVIL 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 informationELECTROMAGNETISM (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 informationGauss 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 informationFrom 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 informationObjects 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 informationCourse Updates. Reminders: 1) Assignment #8 will be able to do after today. 2) Finish Chapter 28 today. 3) Quiz next Friday
Couse Updates http://www.phys.hawaii.edu/~vane/phys272-sp10/physics272.html Remindes: 1) Assignment #8 will be able to do afte today 2) Finish Chapte 28 today 3) Quiz next Fiday 4) Review of 3 ight-hand
More informationPage 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 informationChapter 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 informationANTENNAS. Vector and Scalar Potentials. Maxwell's Equations. D = εe. For a linear, homogeneous, isotropic medium µ and ε are contant.
ANTNNAS Vecto and Scala Potentials Maxwell's quations jωb J + jωd D ρ B (M) (M) (M3) (M4) D ε B Fo a linea, homogeneous, isotopic medium and ε ae contant. Since B, thee exists a vecto A such that B A and
More informationPrepared 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$ 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 informationCurrent, 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 information7.2. Coulomb s Law. The Electric Force
Coulomb s aw Recall that chaged objects attact some objects and epel othes at a distance, without making any contact with those objects Electic foce,, o the foce acting between two chaged objects, is somewhat
More informationPhys-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 informationIn many engineering and other applications, the. variable) will often depend on several other quantities (independent variables).
II PARTIAL DIFFERENTIATION FUNCTIONS OF SEVERAL VARIABLES In man engineeing and othe applications, the behaviou o a cetain quantit dependent vaiable will oten depend on seveal othe quantities independent
More informationVoltage ( = 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 informationEE 5337 Computational Electromagnetics. Maxwell s Equations
9/15/217 Instucto D. Ramond Rumpf (915) 747 6958 cumpf@utep.edu 5337 Computational lectomagnetics Lectue #2 Mawell s quations Lectue 2These notes ma contain copighted mateial obtained unde fai use ules.
More informationGeneral Railgun Function
Geneal ailgun Function An electomagnetic ail gun uses a lage Loentz foce to fie a pojectile. The classic configuation uses two conducting ails with amatue that fits between and closes the cicuit between
More informationReview. 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 informationForce between two parallel current wires and Newton s. third law
Foce between two paallel cuent wies and Newton s thid law Yannan Yang (Shanghai Jinjuan Infomation Science and Technology Co., Ltd.) Abstact: In this pape, the essence of the inteaction between two paallel
More informationPhysics 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 informationElectromagnetic scattering. Graduate Course Electrical Engineering (Communications) 1 st Semester, Sharif University of Technology
Electomagnetic scatteing Gaduate Couse Electical Engineeing (Communications) 1 st Semeste, 1390-1391 Shaif Univesity of Technology Geneal infomation Infomation about the instucto: Instucto: Behzad Rejaei
More informationFields and Waves I Spring 2005 Homework 4. Due 8 March 2005
Homewok 4 Due 8 Mach 005. Inceasing the Beakdown Voltage: This fist question is a mini design poject. You fist step is to find a commecial cable (coaxial o two wie line) fo which you have the following
More informationEKT 345 MICROWAVE ENGINEERING CHAPTER 2: PLANAR TRANSMISSION LINES
EKT 345 MICROWAVE ENGINEERING CHAPTER : PLANAR TRANSMISSION LINES 1 Tansmission Lines A device used to tansfe enegy fom one point to anothe point efficiently Efficiently minimum loss, eflection and close
More informationB. Spherical Wave Propagation
11/8/007 Spheical Wave Popagation notes 1/1 B. Spheical Wave Popagation Evey antenna launches a spheical wave, thus its powe density educes as a function of 1, whee is the distance fom the antenna. We
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 informationFields. Coulomb s Law
Coulomb s Law q t -q q 2 Electic Field Vecto valued function ligned with foce F = q E -q q 2 Supeposition of Electic Field q t -q q 2 Potential Enegy U = U() U() = q du = F d = qe d U = F = qe E d E =
More informationElectrostatics. 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 informationSources of the Magnetic Field. Moving charges currents Ampere s Law Gauss Law in magnetism Magnetic materials
Souces of the Magnetic Field Moving chages cuents Ampee s Law Gauss Law in magnetism Magnetic mateials Biot-Savat Law ˆ ˆ θ ds P db out I db db db db ds ˆ 1 I P db in db db ds sinθ db μ 4 π 0 Ids ˆ B μ0i
More informationev 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 informationObjectives: 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 informationAppendix B The Relativistic Transformation of Forces
Appendix B The Relativistic Tansfomation of oces B. The ou-foce We intoduced the idea of foces in Chapte 3 whee we saw that the change in the fou-momentum pe unit time is given by the expession d d w x
More informationChapter 31 Faraday s Law
Chapte 31 Faaday s Law Change oving --> cuent --> agnetic field (static cuent --> static agnetic field) The souce of agnetic fields is cuent. The souce of electic fields is chage (electic onopole). Altenating
More information