Physics 2102 Jonathan Dowling Physics 2102 Lecture 7

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Physics 2102 Jonathan Dowling Physics 2102 Lecture 7 Capacitors I

Physics 2102 Jonathan Dowling Physics 2102 Lecture 7 Capacitors I

Capacitors and Capacitance Capacitor: any two conductors, one with charge +Q, other with charge

Capacitors and Capacitance Capacitor: any two conductors, one with charge +Q, other with charge –Q –Q Potential DIFFERENCE between +Q Uses: storing and releasing conductors = V electric charge/energy. Q = CV where C = capacitance Most electronic capacitors: micro-Farads (m. F), Units of capacitance: pico-Farads (p. F) — 10– 12 F New technology: Farad (F) = Coulomb/Volt compact 1 F capacitors

Capacitance • Capacitance depends only on GEOMETRICAL factors and on the MATERIAL that separates

Capacitance • Capacitance depends only on GEOMETRICAL factors and on the MATERIAL that separates the two +Q conductors –Q • e. g. Area of conductors, separation, whether the space in between is filled (We first focus on capacitors with air, plastic, etc. where gap is filled by AIR!)

Electrolytic (1940 -70) Electrolytic (new) Paper (1940 -70) Capacitors Variable air, mica Tantalum (1980

Electrolytic (1940 -70) Electrolytic (new) Paper (1940 -70) Capacitors Variable air, mica Tantalum (1980 on) Ceramic (1930 on) Mica (1930 -50

Parallel Plate Capacitor We want capacitance: C=Q/V E field between the plates: (Gauss’ Law)

Parallel Plate Capacitor We want capacitance: C=Q/V E field between the plates: (Gauss’ Law) Relate E to potential difference V: What is the capacitance C ? +Q Area of each plate = A Separation = d charge/area = s = Q/A -Q

Capacitance and Your i. Pod!

Capacitance and Your i. Pod!

Parallel Plate Capacitor — Example • A huge parallel plate capacitor consists of two

Parallel 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 = e 0 A/d = (8. 85 x 10– 12 F/m)(0. 25 m 2)/(0. 001 m) = 2. 21 x 10– 9 F (Very Small!!) Lesson: difficult to get large values of capacitance without special tricks!

Isolated Parallel Plate Capacitor • A parallel plate capacitor of capacitance C is charged

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 is fixed! • C decreases (=e 0 A/d) • Q=CV; V increases. +Q –Q

Parallel Plate Capacitor & Battery • A parallel plate capacitor of capacitance C is

Parallel 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. Does the Electric Field Inside: (a) Increase? (b) Remain the Same? • V is fixed by battery! (c) Decrease? • C decreases (=e 0 A/d) • Q=CV; Q decreases • E = Q/ e 0 A decreases +Q –Q

Spherical Capacitor What is the electric field inside the capacitor? (Gauss’ Law) Relate E

Spherical Capacitor What is the electric field inside the capacitor? (Gauss’ Law) Relate E to potential difference between the plates: Radius of outer plate = b Radius of inner plate = a Concentric spherical shells: Charge +Q on inner shell, –Q on outer shell

Spherical Capacitor What is the capacitance? C = Q/V = Radius of outer plate

Spherical Capacitor What is the capacitance? C = Q/V = Radius of outer plate = b Radius of inner plate = a Concentric spherical shells: Charge +Q on inner shell, –Q on outer shell Isolated sphere: let b >> a,

Cylindrical Capacitor What is the electric field in between the plates? Gauss’ Law! Relate

Cylindrical Capacitor What is the electric field in between the plates? Gauss’ Law! Relate E to potential difference between the plates: Radius of outer plate = b Radius of inner plate = a Length of capacitor = L +Q on inner rod, –Q on outer shell cylindrical Gaussian surface of radius r

Summary • Any two charged conductors form a capacitor. • Capacitance : C= Q/V

Summary • Any two charged conductors form a capacitor. • Capacitance : C= Q/V • Simple Capacitors: Parallel plates: C = e 0 A/d Spherical: C = 4 p e 0 ab/(b-a) Cylindrical: C = 2 p e 0 L/ln(b/a)]

Capacitors in Parallel • A wire is an equipotential surface! • Capacitors in parallel

Capacitors in Parallel • A wire is an equipotential surface! • Capacitors in parallel have SAME potential difference but NOT ALWAYS same charge! • VAB = VCD = V • Qtotal = Q 1 + Q 2 • Ceq. V = C 1 V + C 2 V • Ceq = C 1 + C 2 • Equivalent parallel capacitance = sum of capacitances A C Q 1 C 1 Q 2 C 2 Qtotal B D Ceq

Capacitors in Series Q 1 • Q 1 = Q 2 = Q (WHY?

Capacitors in Series Q 1 • Q 1 = Q 2 = Q (WHY? ? ) • VAC = VAB + VBC Q 2 B A C 1 C 2 Q SERIES: • Q is same for all capacitors • Total potential difference = sum of V C Ceq