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LSU PHYS 2102 - Capacitors

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Slide 1Capacitors and CapacitanceCapacitanceSlide 4Capacitors and CapacitanceParallel Plate CapacitorParallel Plate Capacitor -- exampleIsolated Parallel Plate CapacitorParallel Plate Capacitor & BatterySpherical CapacitorSpherical CapacitorCylindrical CapacitorCylindrical CapacitorSummaryCapacitors in ParallelCapacitors in seriesCapacitors in parallel and in seriesExample 1Example 2Example 3Energy Stored in a CapacitorEnergy Stored in Electric FieldExampleDielectric ConstantExampleExample (soln)SummaryPhysics 2102 Capacitors Physics 2102Gabriela GonzálezCapacitors and CapacitanceCapacitor: any two conductors, one with charge +Q, other with charge -Q+Q-QUses: storing and releasing electric charge/energy. Most electronic capacitors:micro-Farads (mF),pico-Farads (pF) -- 10-12 FNew technology: compact 1 F capacitorsPotential DIFFERENCE between conductors = VQ = CV -- C = capacitanceUnits of capacitance: Farad (F) = Coulomb/VoltCapacitance•Capacitance depends only on GEOMETRICAL factors and on the MATERIAL that separates the two conductors•e.g. Area of conductors, separation, whether the space in between is filled with air, plastic, etc.+Q-Q(We first focus on capacitorswhere gap is filled by AIR!)Electrolytic (1940-70)Electrolytic (new)Paper (1940-70)Tantalum (1980 on)Ceramic (1930 on)Mica(1930-50)Variableair, micaCapacitorsCapacitors and CapacitanceCapacitor: any two conductors, one with charge +Q, other with charge -Q+QUses: storing and releasing electric charge/energy. Most electronic capacitors:micro-Farads (mF),pico-Farads (pF) -- 10-12 FNew technology: compact 1 F capacitorsPotential DIFFERENCE between conductors = VQ = CV C = capacitanceUnits of capacitance: Farad (F) = Coulomb/Volt-QParallel Plate Capacitor+Q-QWhat is the capacitance C?Area of each plate = ASeparation = dcharge/area = s= Q/ARelate E to potential difference V:dxdEV0AQddxAQd000dAVQC0E field between the plates: (Gauss’ Law)AQE00We want capac i t ance: C=Q/VParallel Plate Capacitor -- example•A huge parallel plate capacitor consists of two square metal plates of side 50 cm, separated by an air gap of 1 mm •What is the capacitance?•C = e0A/d = (8.85 x 10-12 F/m)(0.25 m2)/(0.001 m)= 2.21 x 10-9 F(small!!)Lesson: difficult to get large valuesof capacitance without specialtricks!Isolated Parallel Plate Capacitor•A parallel plate capacitor of capacitance C is charged using a battery. •Charge = Q, potential difference = V.•Battery is then disconnected. •If the plate separation is INCREASED, does potential difference V:(a) Increase?(b) Remain the same?(c) Decrease?+Q-Q• Q is fixed!• C decreases (=e0A/d)• Q=CV; V increases.€ C =QV=QEd=ε0AdParallel Plate Capacitor & Battery•A parallel plate capacitor of capacitance C is charged using a battery. •Charge = Q, potential difference = V.•Plate separation is INCREASED while battery remains connected.+Q-Q• V is fixed by battery!• C decreases (=e0A/d)• Q=CV; Q decreases• E = Q/ e0A decreasesDoes the electric field inside:(a) Increase?(b) Remain the same?(c) Decrease?€ C =QV=QEd=ε0AdSpherical CapacitorWhat is the electric field insidethe capacitor? (Gauss’ Law)Radius of outer plate = bRadius of inner plate = aConcentric spherical shells:Charge +Q on inner shell,-Q on outer shellRelate E to potential differencebetween the plates:204 rQEbardEVbabarkQdrrkQ2bakQ11Spherical CapacitorWhat is the capacitance?C = Q/V =Radius of outer plate = bRadius of inner plate = aConcentric spherical shells:Charge +Q on inner shell,-Q on outer shellIsolated sphere: let b >> a,baQQ1140)(40ababaC04Cylindrical CapacitorWhat is the electric field in between the plates?Relate E to potential differencebetween the plates:Radius of outer plate = bRadius of inner plate = acylindrical surface of radius rLength of capacitor = L+Q on inner rod, -Q on outer shellrLQE02bardEVbabaLrQdrrLQ002ln2abLQln20Cylindrical CapacitorWhat is the capacitance C?C = Q/V =Radius of outer plate = bRadius of inner plate = aLength of capacitor = LCharge +Q on inner rod,-Q on outer shellabLQQln20abLln20Example: co-axial cable.Summary• Any two charged conductors form a capacitor.•Capacitance : C= Q/V•Simple Capacitors:Parallel plates: C = e0 A/dSpherical : C = 4p e0 ab/(b-a)Cylindrical: C = 2p e0 L/ln(b/a)Capacitors in Parallel•A wire is a conductor, so it is an equipotential.•Capacitors in parallel have SAME potential difference but NOT ALWAYS same charge.•VAB = VCD = V •Qtotal = Q1 + Q2•CeqV = C1V + C2V•Ceq = C1 + C2•Equivalent parallel capacitance = sum of capacitancesA BCDC1C2Q1Q2CeqQtotalPARALLEL: • V is same for all capacitors• Total charge in Ceq = sum of chargesCapacitors in series•Q1 = Q2 = Q (WHY??) •VAC = VAB + VBCAB CC1C2Q1Q2CeqQ21CQCQCQeq21111CCCeqSERIES: • Q is same for all capacitors• Total potential difference in Ceq = sum of VCapacitors in parallel and in series•In series : –1/Ceq = 1/C1 + 1/C2–Veq=V1 +V2–Qeq=Q1=Q2C1C2Q1Q2C1C2Q1Q2•In parallel : –Ceq = C1 + C2–Veq=V1=V2–Qeq=Q1+Q2CeqQeqExample 1What is the charge on each capacitor?10 mF30 mF20 mF120V• Q = CV; V = 120 V• Q1 = (10 mF)(120V) = 1200 mC • Q2 = (20 mF)(120V) = 2400 mC• Q3 = (30 mF)(120V) = 3600 mCNote that:•Total charge (7200 mC) is shared between the 3 capacitors in the ratio C1:C2:C3 -- i.e. 1:2:3Example 2What is the potential difference across each capacitor?10 mF30 mF20 mF120V• Q = CV; Q is same for all capacitors• Combined C is given by:)30(1)20(1)10(11FFFCeq• Ceq = 5.46 mF• Q = CV = (5.46 mF)(120V) = 655 mC• V1= Q/C1 = (655 mC)/(10 mF) = 65.5 V• V2= Q/C2 = (655 mC)/(20 mF) = 32.75 V• V3= Q/C3 = (655 mC)/(30 mF) = 21.8 VNote: 120V is shared in the ratio of INVERSE capacitances i.e.1:(1/2):(1/3) (largest C gets smallest V)Example 3In the circuit shown, what is the charge on the 10F capacitor?10 mF10 mF10V10 mF5 mF5 mF10V•The two 5F capacitors are in parallel•Replace by 10F •Then, we have two 10F capacitors in series•So, there is 5V across the 10F capacitor of interest•Hence, Q = (10F )(5V) = 50CEnergy Stored in a Capacitor•Start out with uncharged


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