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Gauss LAW

The document covers Gauss' law and electric flux in detail, emphasizing the relationship between electric field lines, surface area, and charge. It explains how to calculate electric flux through various surfaces and applies Gauss' law to different charge distributions, including point charges and continuous charge distributions. Key examples illustrate the application of Gauss' law to spherical and cylindrical geometries, highlighting the behavior of electric fields in and around charged conductors.

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Fall 2008Physics 231 Lecture 2-1 Gauss’ Law
Fall 2008Physics 231 Lecture 2-2 Topic : Gauss’ Law By Prof . AJAL A. J Head of Academics
Fall 2008Physics 231 Lecture 2-3 Electric Field Lines The number of field lines, also known as lines of force, are related to strength of the electric field More appropriately it is the number of field lines crossing through a given surface that is related to the electric field
Fall 2008Physics 231 Lecture 2-4 Flux How much of something passes through some surface Number of particles passing through a given surface Two ways to define Number per unit area (e.g., 10 particles/cm2) Number passing through an area of interest
Fall 2008Physics 231 Lecture 2-5 Electric Flux The electric flux is defined to be AEE  Where E is the electric field and A is the area
Fall 2008Physics 231 Lecture 2-6 Electric Flux If surface area is not perpendicular to the electric field we have to slightly change our definition of the flux cosAEE  Where  is the angle between the field and the unit vector that is perpendicular to the surface
Fall 2008Physics 231 Lecture 2-7 Electric Flux We can see that the relationship between the flux and the electric field and the area vector is just the dot product of two vectors nAE AE E E ˆ    nˆ is a unit vector perpendicular to the surface
Fall 2008Physics 231 Lecture 2-8 A Convention The direction of a unit vector for an open surface is ambiguous For a closed surface, the unit vector is taken as being pointed outward
Fall 2008Physics 231 Lecture 2-9 Electric Flux Where flux lines enter the surface, the surface normal and the electric field lines are anti-parallel Where the flux lines exit the surface they are parallel
Fall 2008Physics 231 Lecture 2-10 Electric Flux Is there a difference in the net flux through the cube between the two situations? No! It is important to remember to properly take into account the various dot products
Fall 2008Physics 231 Lecture 2-11 Electric Flux The equation we have for flux is fine for simple situations the electric field is uniform and the surface area is plane What happens when either one or the other or both is not true
Fall 2008Physics 231 Lecture 2-12 Electric Flux We proceed as we did in the transition from discrete charges to a continuous distribution of charges We break the surface area into small pieces and then calculate the flux through each piece and then sum them In the limit of infinitesimal areas this just becomes an integral   AdEE 
Fall 2008Physics 231 Lecture 2-13 Electric Flux of a Point Charge What is electric flux that comes from a point charge? We start from   AdEE  2 04 1 r q E   Since E is radial, its dot product with the differential area vector, which is also radial, is always one The electric field is given by Also E is the same at every point on the surface of the sphere The problem has spherical symmetry, we therefore use a sphere as the Gaussian surface
Fall 2008Physics 231 Lecture 2-14 Electric Flux of a Point Charge The integral over the surface area of the sphere yields 2 4 rA   dAEE For these reasons, E can be pulled out from the integral and what remains is Pulling all this together then yields 0 2 2 0 4 4 1 ;    q r r q EA E EE   Notice that this is independent of the radius of the sphere
Fall 2008Physics 231 Lecture 2-15 A positive charge is contained inside a spherical shell. How does the differential electric flux, dФE, through the surface element dS change when the charge is moved from position 1 to position 2? dФE a) increases b) decreases c) doesn’t change dS 1 dS 2 Example 1
Fall 2008Physics 231 Lecture 2-16 dS 1 dS 2 Example 1 - continued The total flux of a charge is constant, with the density of flux lines being higher the closer you are to the charge Therefore as you move the charge closer to the surface element, the density of flux lines increases Multiplying this higher density by the same value for the area of dS gives us that the incremental flux also increases dФE a) increases b) decreases c) doesn’t change
Fall 2008Physics 231 Lecture 2-17 dS 1 dS 2 A positive charge is contained inside a spherical shell. How does the total flux, ФE, through the entire surface change when the charge is moved from position 1 to position 2? a) ФE increases b) ФE decreases c) ФE doesn’t change Example 2 As we previously calculated, the total flux from a point charge depends only upon the charge
Fall 2008Physics 231 Lecture 2-18 Gauss’ Law  i iE q 0 1  The result for a single charge can be extended to systems consisting of more than one charge One repeats the calculation for each of the charges enclosed by the surface and then sum the individual fluxes Gauss’ Law relates the flux through a closed surface to charge within that surface
Fall 2008Physics 231 Lecture 2-19 Gauss’ Law 0 net E Q AdE    Gauss’ Law states that The net flux through any closed surface equals the net (total) charge inside that surface divided by 0 Note that the integral is over a closed surface
Fall 2008Physics 231 Lecture 2-20 A B A blue sphere A is contained within a red spherical shell B. There is a charge QA on the blue sphere and charge QB on the red spherical shell. The electric field in the region between the spheres is completely independent of QB the charge on the red spherical shell. True False Example 3
Fall 2008Physics 231 Lecture 2-21 Surfaces Choose surface appropriate to problem It does not have to be a sphere Exploit symmetries, if any
Fall 2008Physics 231 Lecture 2-22 Example 4 Thin Infinite Sheet of Charge A given sheet has a charge density given by s C/m2 By symmetry, E is perpendicular to the sheet Use a surface that exploits this fact A cylinder A Gaussian pillbox E
Fall 2008Physics 231 Lecture 2-23 Thin Infinite Sheet of Charge But E and Acurved are perpendicular to each other so their dot product is zero and the middle term on the left disappears 0 0  s  s A AEEAAE A AdE rightcurvedleft      0 0 2 2  s  s   E A AE
Fall 2008Physics 231 Lecture 2-24 Example 5 Infinite Line having a Charge Density l Apply Gauss’ Law: Equating these and rearranging yields h + + + + y + + + + + Er Er + + + + + + + ++ + + + + + By Symmetry Therefore, choose the Gaussian surface to be a cylinder of radius r and length h aligned with the x-axis On the ends, 0 SdE  since E// is zero andOn the barrel, rhESdE 2  hq l r E 02 l  This is the same result as using the integral formulation E-field must be  to line of charge and can only depend on distance from the line
Fall 2008Physics 231 Lecture 2-25 Example 6 Solid Uniformly Charged Sphere A charge Q is uniformly distributed throughout the volume of an insulating sphere of radius R. 3/3 R4 Q :DensityCharge    Now select a Gaussian sphere of radius r within this larger sphere What is the electric field for r < R? Calculate average charge density Charge within this sphere is given by 3 3 3 3 3 4 34 R r Qr R Q VQ enclencl                   /
Fall 2008Physics 231 Lecture 2-26 Electric Field is everywhere perpendicular to surface, i.e. parallel to surface normal Example 6 Solid Uniformly Charged Sphere Gauss’ Law then gives 3 0 3 3 0 2 0 4 4 R rQ E R rQ rE Q AdE encl         Field increases linearly within sphere Outside of sphere, electric field is given by that of a point charge of value Q
Fall 2008Physics 231 Lecture 2-27 Charges on Conductors Given a solid conductor, on which is placed an excess charge then in the static limit The excess charge will reside on the surface of the conductor and Everywhere the electric field due to this excess charge will be perpendicular to the surface and The electric field within the conductor will everywhere be zero
Fall 2008Physics 231 Lecture 2-28 Example 7 1. How is the charge distributed on the sphere? 2. How is the charge distributed on the spherical shell? 3. What is the electric field at r < R1? Between R1 and R2?At r > R2? 4. What happens when you connect the two spheres with a wire? (What are the charges?) The inner sphere carries a charge Q1, and the spherical shell carries a charge Q2, such that Q2 = - 3 Q1 A solid conducting sphere is concentric with a thin conducting shell, as shown
Fall 2008Physics 231 Lecture 2-29 1. How is the charge distributed on the sphere? Remember that the electric field inside a conductor in a static situation is zero. By Gauss’s Law, there can be no net charge inside the conductor + + + + + + + + The charge, Q1, must reside on the outside surface of the sphere
Fall 2008Physics 231 Lecture 2-30 2. How is the charge distributed on the spherical shell? The electric field inside the conducting shell is zero. The charges are distributed uniformly over the inner and outer surfaces of the shell, hence and2 2 1 4 R Q inner  s  2 2 1 2 2 12 4 2 4 R Q R QQ outer  s     There can be no net charge inside the conductor Using Gauss’ Law it can be shown that the inner surface of the shell must carry a net charge of -Q1 The outer surface must carry the charge +Q1 + Q2, so that the net charge on the shell equals Q2
Fall 2008Physics 231 Lecture 2-31 r < R1: This is inside the conducting sphere, therefore The electric field inside a conductor is zero. Between R1 and R2 : R1 < r < R2 Charge enclosed within a Gaussian sphere = Q1 r > R2 Charge enclosed within a Gaussian sphere = Q1 + Q2 3. What is the Electric Field at r < R1? Between R1 and R2? At r > R2? 0E  r r Q kE ˆ2 1  r r Q kr r QQ kr r QQ kE ˆ 2 ˆ 3 ˆ 2 1 2 11 2 21      
Fall 2008Physics 231 Lecture 2-32 4. What happens when you connect the two spheres with a wire? (What are the charges?) The charge Q1 + Q2 resides on the outer surface Also, for r < R2 and for r > R2 After electrostatic equilibrium is reached, there is no charge on the inner sphere, and none on the inner surface of the shell r r Q kE ˆ 2 2 1  0E 
Fall 2008Physics 231 Lecture 2-33 ii) How is the charge distributed on the cavity wall? (a) Uniformly (b) More charge closer to –q (c) Less charge closer to -q Example 8 iii) How is the charge distributed on the outside of the sphere? (a) Uniformly (b) More charge near the cavity (c) Less charge near the cavity -q An uncharged spherical conductor has a weirdly shaped cavity carved out of it. Inside the cavity is a charge -q. (a) Less than q (b) Exactly q (c) More than q i) How much charge is on the cavity wall?
Fall 2008Physics 231 Lecture 2-34 By Gauss’ Law, since E = 0 inside the conductor, the total charge on the inner wall must be q (and therefore -q must be on the outside surface of the conductor, since it has no net charge). -q Example 8 An uncharged spherical conductor has a weirdly shaped cavity carved out of it. Inside the cavity is a charge -q. (a) Less than< q (b) Exactly q (c) More than q i) How much charge is on the cavity wall?
Fall 2008Physics 231 Lecture 2-35 Example 8 An uncharged spherical conductor has a weirdly shaped cavity carved out of it. Inside the cavity is a charge -q. ii) How is the charge distributed on the cavity wall? (a) Uniformly (b) More charge closer to –q (c) Less charge closer to -q The induced charge will distribute itself non-uniformly to exactly cancel everywhere in the conductor. The surface charge density will be higher near the -q charge. E  -q
Fall 2008Physics 231 Lecture 2-36 The charge will be uniformly distributed (because the outer surface is symmetric). Outside the conductor, the E field always points directly to the center of the sphere, regardless of the cavity or charge or its location. Note: this is why your radio, cell phone, etc. won’t work inside a metal building! Example 8 An uncharged spherical conductor has a weirdly shaped cavity carved out of it. Inside the cavity is a charge -q. iii) How is the charge distributed on the outside of the sphere? (a) Uniformly (b) More charge near the cavity (c) Less charge near the cavity -q