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Gauss's Law for Electric Field Gauss’s Law for Electric Field The net electric flux ΦE through any closed surface is equal to the net charge Qin inside divided by the permittivity constant ǫ0: Qin Qin −12 2 −1 −2 E~ · dA~ = 4πkQin = i.e. ΦE = with ǫ0 = 8.854 × 10 C N m ǫ ǫ I 0 0 The closed surface can be real or fictitious. It is called “Gaussian surface”. The symbol denotes an integral over a closed surface in this context. H • Gauss’s law is a general relation between electric charge and electric field. • In electrostatics: Gauss’s law is equivalent to Coulomb’s law. • Gauss’s law is one of four Maxwell’s equations that govern cause and effect in electricity and magnetism. 1/9/2015 [tsl44 – 1/32] Gauss’ Law for Electric Field (Illustration) 1/9/2015 [tsl445 – 2/32] Gaussian surface problem (1) (A) The electric fluxes through the Gaussian surfaces SA and SB are ΦE = 5C/ǫ0 and (B) ΦE = 3C/ǫ0, respectively. SB SA q1 q2 Find the electric charges q1 and q2. 1/9/2015 [tsl45 – 3/32] Gaussian surface problem (2) (A) The electric fluxes through the Gaussian surfaces SA and SB are ΦE = 1C/ǫ0 and (B) ΦE = 3C/ǫ0, respectively. SA SB q q1 =2C 2 q3 Find the electric charges q2 and q3. 1/9/2015 [tsl46 – 4/32] Gaussian surface problem (3) A proton, a neutron, and an electron are placed in different boxes. The electric fluxes through the three Gaussian surfaces are as indicated. ε ε e/ 0 e/ 0 zero A BC Name the particle in each box. 1/9/2015 [tsl47 – 5/32] Gaussian surface problem (4) Three point charges q1, q2, q3 produce electric fluxes through the three Gaussian surfaces as indicated. ε ε 2C/ 0 1C/ 0 q 2 q q 1 3 ε 5C/ 0 (a) Find the net charge Q = q1 + q2 + q3. (b) Find the individual charges q1, q2, q3. 1/9/2015 [tsl48 – 6/32] Gaussian surface problem (5) A positive charge and a negative charge are placed in different boxes. One box remains empty. The electric fluxes through the three Gaussian surfaces are as indicated. ε ε −4C/ 0 +2C/ 0 A B C ε −2C/ 0 (a) Which box contains the positive charge? (b) Which box contains the negative charge? 1/9/2015 [tsl49 – 7/32] Gaussian surface problem (6) (A) The electric fluxes through the Gaussian surfaces SA, SB, and SC are ΦE = 4C/ǫ0, (B) (C) ΦE = 1C/ǫ0, and ΦE = 2C/ǫ0, respectively. SC SA SB q q1 2 q3 Find the electric charges q1, q2, and q3. 1/9/2015 [tsl50 – 8/32] Calculating E~ from Gauss’s Law: Strategy Design the Gaussian surface such that it reflects the symmetry of the problem at hand. • Use concentric Gaussian spheres in problems with spherically symmetric charge distributions. The electric field is perpendicular to the Gaussian sphere (E~ k dA~). • Use coaxial Gaussian cylinders in problems with cylindrically symmetric charge distributions. The electric field is perpendicular to the curved surface (E~ k dA~) and parallel to the flat surfaces (E~ ⊥ dA~). • Use Gaussian cylinders with axis perpendicular to planar charge distributions. The electric field is parallel to the curved surface (E~ ⊥ dA~) and perpendicular to the flat surfaces (E~ k dA~). 1/9/2015 [tsl51 – 9/32] Calculating E~ from Gauss’s Law: Point Charge • Consider a positive point charge Q. • Use a Gaussian sphere of radius R centered at the location of Q. • Surface area of sphere: A = 4πR2. 2 • Electric flux through Gaussian surface: ΦE = E~ · dA~ = E(4πR ). I • Net charge inside Gaussian surface: Qin = Q. Qin Q • Gauss’s law E~ · dA~ = becomes E(4πR2)= . ǫ ǫ I 0 0 1 Q kQ • Electric field at radius R: E = = . 2 2 4πǫ0 R R 1/9/2015 [tsl52 – 10/32] Calculating E~ from Gauss’s Law: Charged Wire • Consider a uniformly charged wire of infinite length. • Charge per unit length on wire: λ (here assumed positive). • Use a coaxial Gaussian cylinder of radius R and length L. • Electric flux through Gaussian surface: ΦE = E~ · dA~ = E(2πRL). I • Net charge charge inside Gaussian surface: Qin = λL. Qin λL • Gauss’s law E~ · dA~ = becomes E(2πRL)= . ǫ ǫ I 0 0 1 λ • Electric field at radius R: E = . 2πǫ0 R 1/9/2015 [tsl53 – 11/32] Calculating E~ from Gauss’s Law: Charged Plane Sheet • Consider a uniformly charged plane sheet. • Charge per unit area on sheet: σ (here assumed positive). • Use Gaussian cylinder with cross-sectional area A placed as shown. • Electric flux through Gaussian surface: ΦE = E~ · dA~ = 2EA. I Net charge charge inside Gaussian surface: Qin = σA. Qin σA • Gauss’s law E~ · dA~ = becomes 2EA = . ǫ ǫ I 0 0 σ • Electric field at both ends of cylinder: E = 2ǫ0 (pointing away from sheet). • Note that E does not depend on the distance from the sheet. 1/9/2015 [tsl54 – 12/32] Calculating E~ from Gauss’s Law: Charged Slab • Consider a uniformly charged slab. • Charge per unit volume on slab: ρ. • Use Gaussian cylinder as shown. • Total electric flux: ΦE = 2|Ez|A. 2ρA|z| (|z|≤ a) • Net charge inside: Qin = ( 2ρAa (|z|≥ a) 2ρA|z| ǫ0 (|z|≤ a) • Gauss’s law: 2|Ez|A = 2ρAa ( ǫ0 (|z|≥ a) ρa − ǫ0 (z ≤−a) • Electric field: E = ρz (−a ≤ z ≤ a) z 8 ǫ0 > ρa < ǫ0 (z ≥ a) :> 1/9/2015 [tsl373 – 13/32] Electric Field of Uniformly Charged Spherical Shell • Radius of charged spherical shell: R • Electric charge on spherical shell: Q = σA = 4πσR2. • Use a concentric Gaussian sphere of radius r. Q • r > R: E(4πr2)= ǫ0 1 Q ⇒ E = 2 4πǫ0 r Qin • r < R: E(4πr2)= = 0 ǫ0 ⇒ E = 0 1/9/2015 [tsl55 – 14/32] Electric Field of Uniformly Charged Solid Sphere • Radius of charged solid sphere: R • Electric charge on sphere: 4π Q = ρV = ρR3. 3 • Use a concentric Gaussian sphere of radius r. Q • r > R: E(4πr2)= ǫ0 1 Q ⇒ E = 2 4πǫ0 r 1 4π • r < R: E(4πr2)= r3ρ ǫ 3 0 „ « ρ 1 Q ⇒ E(r)= r = r 3 3ǫ0 4πǫ0 R 1/9/2015 [tsl56 – 15/32] Electric Field of Oppositely Charged Infinite Sheets • Consider two infinite sheets of charge with charge per unit area ±σ, respectively. • The sheets are positioned at x = 0 and x = 2m, respectively. σ • Magnitude of field produced by each sheet: E = . 2ǫ0 (+) (−) σ σ • Electric field at x< 0: Ex = Ex + Ex = − + = 0. 2ǫ0 2ǫ0 (+) (−) σ σ σ • Electric field at 0 <x< 2m: Ex = Ex + Ex =+ + = . 2ǫ0 2ǫ0 ǫ0 (+) (−) σ σ • Electric field at x> 2m: Ex = Ex + Ex =+ − = 0. 2ǫ0 2ǫ0 1/9/2015 [tsl57 – 16/32] Electric Field Near Charged Infinite Sheets Consider three pairs of parallel, infinite, uniformly charged sheets. The charge per unit area is equal in magnitude on all sheets. Find the direction (↑, ↓, none) of the electric field at the nine locations indicated. E1 E 4 E 7 σ > 0 σ < 0 σ > 0 E 2 E 5 E 8 σ > 0 σ < 0 σ < 0 E E 3 E 6 9 1/9/2015 [tsl446 – 17/32] Unit Exam I: Problem #2 (Spring ’09) Consider two very large uniformly charged parallel sheets as shown. The charge densities are −12 −2 −12 −2 σA = +7 × 10 Cm and σB = −4 × 10 Cm , respectively. Find magnitude and direction (left/right) of the electric fields E1, E2, and E3. EE1 2 E3 σ Α σΒ 1/9/2015 [tsl390 – 18/32] Unit Exam I: Problem #2 (Spring ’09) Consider two very large uniformly charged parallel sheets as shown. The charge densities are −12 −2 −12 −2 σA = +7 × 10 Cm and σB = −4 × 10 Cm , respectively. Find magnitude and direction (left/right) of the electric fields E1, E2, and E3. EE1 2 E3 Solution: σ Α σΒ |σA| EA = = 0.40N/C (directed away from sheet A). 2ǫ0 1/9/2015 [tsl390 – 18/32] Unit Exam I: Problem #2 (Spring ’09) Consider two very large uniformly charged parallel sheets as shown. The charge densities are −12 −2 −12 −2 σA = +7 × 10 Cm and σB = −4 × 10 Cm , respectively. Find magnitude and direction (left/right) of the electric fields E1, E2, and E3. EE1 2 E3 Solution: σ Α σΒ |σA| EA = = 0.40N/C (directed away from sheet A). 2ǫ0 |σB| EB = = 0.23N/C (directed toward sheet B). 2ǫ0 1/9/2015 [tsl390 – 18/32] Unit Exam I: Problem #2 (Spring ’09) Consider two very large uniformly charged parallel sheets as shown. The charge densities are −12 −2 −12 −2 σA = +7 × 10 Cm and σB = −4 × 10 Cm , respectively. Find magnitude and direction (left/right) of the electric fields E1, E2, and E3. EE1 2 E3 Solution: σ Α σΒ |σA| EA = = 0.40N/C (directed away from sheet A). 2ǫ0 |σB| EB = = 0.23N/C (directed toward sheet B). 2ǫ0 E1 = EA − EB = 0.17N/C (directed left). 1/9/2015 [tsl390 – 18/32] Unit Exam I: Problem #2 (Spring ’09) Consider two very large uniformly charged parallel sheets as shown. The charge densities are −12 −2 −12 −2 σA = +7 × 10 Cm and σB = −4 × 10 Cm , respectively. Find magnitude and direction (left/right) of the electric fields E1, E2, and E3. EE1 2 E3 Solution: σ Α σΒ |σA| EA = = 0.40N/C (directed away from sheet A). 2ǫ0 |σB| EB = = 0.23N/C (directed toward sheet B). 2ǫ0 E1 = EA − EB = 0.17N/C (directed left). E2 = EA + EB = 0.63N/C (directed right).
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