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ELECTRICITY AND MAGNETISM P10D Coulomb’s Law The force of attraction or repulsion between two point charges q1 and q2 is directly proportional to the product of their charges and inversely proportional to the square of the distance between them. where F12 is the force exerted on point charge q1 by point charge q2 when they are separated by a distance r12. The unit vector is directed from q2 to q1 along the line between the two charges. The constant is called the permitivity of free space. In SI units where force is in Newtons (N), distance in meters (m) and charge in coulombs (C), Coulomb’s law and the Principle of Superposition constitute the physical input for electrostatics. The force on any one charge due to a collection of other charges is the vector sum of the forces due to each individual charge. Here Problem Solving Strategies: 1. Draw a clear diagram of the situation. Be sure to distinguish between the fixed external charges and the charges which the forces must be found. The diagram should contain the coordinate axes for reference. 2. Electric force is a vector quantity; when many forces are present the net force is a vector sum. 3. Search for symmetries in the distribution of charges that give rise to the electric force. When symmetries are present, the net force along certain directions will be zero. Example: Consider three point charges q1 = q2 = 2.0 C and q3 = -3 C which are placed as shown. Calculate the net force on q1 and q3. The force on q1 is F1 = F12 + F13. Similarly, F3 = F31 + F32 Electric Field. Electric field is defined as the electric force per unit charge. The direction of the field is taken to be the direction of the force it would exert on a positive test charge. The electric field is radially outward from a positive charge and radially in toward a negative point charge. The electric field can be defined by measuring the magnitude and direction of the electric force F on a test charge q0. A small test charge is used so as not to interfere with the field distribution of the other charges. Thus we define the electric field as . The SI unit of electric field is NC-1. For a point charge, Electric Field Concepts Field Line Diagrams: A convenient way to visualize the electric field due to any charge distribution is to draw a field line diagram. At any point the field line has the same direction as the electric field vector Electric field lines diverge from positive charges and converge into negative charges. Rules for constructing filed lines: 1. Field lines begin at positive charge and end at negative charge 2. The number of field lines shown diverging from or converging into a point is proportional to the magnitude of the charge. 3. Field lines are spherically symmetric near a point charge 4. If the system has a net charge, the field lines are spherically symmetric at great distances 5. Field lines never cross each other. The Electric Dipole and their Electric Fields An electric dipole consists of two charges + q and –q, of equal magnitude but opposite sign, that are separated by a distance L. From the diagram, E = Ex i = (E1x + E2x)i = 2E1x i where . But Hence I Define the product p = qL as the electric dipole moment. We make p = qL a vector by defining L to be directed from –q to +q. The vector p points from the negative charge to the positive charge. The electric field decreases with r as 1/r3. Finally, . If r >>L, then and Electric Dipole Field: Charge Distributions: The simplest kind of charge distribution is an isolated point charge (i.e., an amount of charge covering such a small region of space that we need not be concerned about its dimensions). When the finite size of the space occupied by a collection of charges must be considered, it is useful to consider the density of charge. The word density is used is used in three different ways. (rho) for the charge per unit volume, the volume density (sigma) for the charge per unit area, the area density (lambda) for the charge per unit length, the linear density Thus we can write Cm-3, Cm-2, Cm-1. Find the electric field a distance z above the midpoint of a straight line segment of length 2L which carries a uniform line charge . (Model of a transmission line) It is advantageous to chop the line up into symmetrically placed pairs (at x). Here where q is the total charge on the rod The horizontal components of the two fields cancel. The net field of the pair is Here , and x runs from 0 to L How to evaluate this integral Consider ; Let , then and . Substitute these into the integral: From diagram, Hence Substitute the limits x = 0 and x = L to get the desired answer. For points far from the line ( z >> L), this result simplifies to . The line “looks” like a point charge , so the field reduces to that of a point charge . Find the electric field a distance z above one end of a straight line segment of length L, which carries a uniform line charge . (Model of a transmission line) Net electric field E = Ex + Ez For z >> L and , Find the electric field a distance z above the center of a circular loop of radius R, which carries a uniform line charge . Here, where q is the total charge of the loop Horizontal components cancel, leaving: (both constants) But Find the electric field a distance z above the center of a flat circular disk of radius a, which carries a uniform surface density, . (Models an electrostatic microphone) A typical element is a ring of radius r and thickness dr, which has an area . The charge density on the disk is . The charge on the element is: The electric field at P produced by this ring is Since we have expressed a positive ring thickness as dr, we sum the rings from the center toward the edge. That is, the radius ranges from 0 to a. . Let , then du = 2r dr, and So When z << a, When z >> a, which is the expected result for a point charge located at the origin. Gauss’ Law: The net flux through any closed surface is proportional to the net charge enclosed by that surface, i.e., The total of the electric flux out of a closed surface is equal to the charge enclosed divided by the permittivity. The electric flux through an area is defined as the electric field multiplied by the area of the surface projected in a plane perpendicular to the field. Gauss's Law is a general law applying to any closed surface. It is an important tool since it permits the assessment of the amount of enclosed charge by mapping the field on a surface outside the charge distribution. For geometries of sufficient symmetry, it simplifies the calculation of the electric field. Gauss' Law, Integral Form The area integral of the electric field over any closed surface is equal to the net charge enclosed in the surface divided by the permittivity of space. Gauss' law is a form of one of Maxwell's equations, the four fundamental equations for electricity and magnetism. Gauss' law permits the evaluation of the electric field in many practical situations by forming a symmetric Gaussian surface surrounding a charge distribution and evaluating the electric flux through that surface. Flux and Gauss's Law Example: Water Flow Suppose water flows through a square surface of area A with a uniform velocity . We want to define flux as the amount of water that flows through the surface per second. First, notice that the flux depends on the direction of the velocity vector relative to the surface. Questions Compare the water flux in the following three situations. Rank the flux in cases (a), (b), and (c), from largest to smallest. (a) is perpendicular to the surface (b) is at a 45 degree angle to the surface (c) is parallel to the surface If the biggest flux is 1, what is the relative number corresponding to the flux in the other two cases? Answer (a): 1 (b): (c): 0 Electric Flux The concept of electric flux is useful in association with Gauss' law. The electric flux through a planar area is defined as the electric field times the component of the area perpendicular to the field. If the area is not planar, then the evaluation of the flux generally requires an area integral since the angle will be continually changing. When the area A is used in a vector operation like this, it is understood that the magnitude of the vector is equal to the area and the direction of the vector is perpendicular to the area. Gaussian Surface: Part of the power of Gauss' law in evaluating electric fields is that it applies to any surface. It is often convenient to construct an imaginary surface called a Gaussian surface to take advantage of the symmetry of the physical situation. Conductor at Equilibrium For a conductor at equilibrium: 1. The net electric charge of a conductor resides entirely on its surface. (The mutual repulsion of like charges from Coulomb's Law demands that the charges be as far apart as possible, hence on the surface of the conductor.) 2. The electric field inside the conductor is zero. (Any net electric field in the conductor would cause charge to move since it is abundant and mobile. This violates the condition of equilibrium: net force =0.) 3. The external electric field at the surface of the conductor is perpendicular to that surface. (If there were a field component parallel to the surface, it would cause mobile charge to move along the surface, in violation of the assumption of equilibrium.) Electric Field: Conductor Surface Examining the nature of the electric field near a conducting surface is an important application of Gauss' law. Considering a cylindrical Gaussian surface oriented perpendicular to the surface, it can be seen that the only contribution to the electric flux is through the top of the Gaussian surface. The flux is given by The fact that the conductor is at equilibrium is an important constraint in this problem. It tells us that the field is perpendicular to the surface, because otherwise it would exert a force parallel to the surface and produce and the electric field is simply charge motion. Likewise it tells us that the field in the interior of the conductor is zero, since otherwise charge would be moving and not at equilibrium. While strictly true only for an infinite conductor, it tells us the limiting value as we approach any conductor at equilibrium. Gauss's Law for a Single Point Charge Gauss's Law applies to any charge contribution, but let us apply it now to the simplest case, that of a single point charge q. Construct a spherical Gaussian surface of radius r around the charge q. Take a small area on the Gaussian surface. The area vector dA points radially outward, as does the electric field vector at this point. Therefore, the electric flux through this small area is From the spherical symmetry, all of such small area elements contribute equally to the total. According to Gauss's Law, because = q. Solving for the electric field gives which is just Coulomb's Law! A Uniformly Charged Solid Sphere An insulating sphere of radius R has a total charge q uniformly distributed throughout its volume. We want to find the electric field everywhere, that is, at an inside point r < R, and also at an outside point r > R. For the case where r < R: We construct a spherical Gaussian surface of radius r and apply Gauss's Law. We already know that for a spherically symmetric case, . We have to be careful about qenc, though. qenc is the net charge within the Gaussian surface, not the total charge q of the entire sphere. For this reason, we need to multiply the total charge by the ratio of the volume of the Gaussian surface to the volume of the entire sphere: Therefore, For the case where r > R: We construct a spherical Gaussian surface through an outside point r > R, and apply Gauss's Law. In this case, The graph below is of the magnitude of the electric field due to a uniformly charged sphere, plotted as a function of distance from the center of the sphere. Electric Field for a Charged Sheet What is the electric field due to a large, thin charged sheet made of some nonconducting material? We construct a cylindrical Gaussian surface, and place it symmetrically in the charged sheet as shown in the above figure. Let the area of each top surface of the cylinder be A, and the surface charge density on the sheet be . Applying Gauss's Law to this cylindrical Gaussian surface gives and we note qenc = A. Therefore, Electric Field between Capacitor Plates Consider two large, parallel conducting plates, one with a charge density + and the other with charge density - . The two opposite charges are attracted to the inside of the plates, as shown. We construct a cylindrical Gaussian surface, with one base area within a conducting plate and another base between the plates. If the area of each base is A, then we have where E is the electric field at the base located between the parallel plates, since E = 0 on the base inside the conductor plate. Then, we have Electric Field Due to a Line Charge Consider an infinitely long straight line charge with linear charge density , which is in units of Coulombs per meter. Choose a cylinder because it mimics the symmetry of the wire. We construct a cylindrical Gaussian surface of radius r and length L. The electric flux about this Gaussian surface is Therefore, Question Find the electric field at all points due to a long, solid cylinder of radius R and uniform charge density . AnswerB Begin by choosing an appropriate Gaussian surface: one that mimics the symmetry of the case. Therefore, since we are concerned with a long cylinder, we choose a Gaussian surface that is also a long cylinder. To find the field everywhere, we need to examine two cases: when the radius r of the Gaussian surface is less than R, and when r > R. Case I: r < R We note that the electric field will be constant everywhere on the cylindrical Gaussian surface; we also note that this surface has a surface area of 2 rL. Thus, Gauss's Law becomes The uniform charge density of the cylinder is . Therefore, the enclosed charge qenc is simply times the volume enclosed by the Gaussian surface, r2L. This gives us Therefore, for r < R, Case II: r > R Again, the electric field will be constant everywhere on the cylindrical Gaussian surface, and the surface area of that surface is still 2 rL. With r > R, the entire cylinder is enclosed, so qenc is equal to the uniform charge density times the volume of the charged cylinder, R2L. This gives us Therefore, for r > R, To summarize, here is a plot of the electric field versus the radius r of the Gaussian surface for this problem: A Uniformly Charged Sphere Question Use Gauss's Law to find the electric field everywhere due to a uniformly charged insulator shell, like the one shown below. The shell has a total charge Q, which is uniformly distributed throughout its volume. (a) What is the charge on the inner surface of the conductor? (b) What is the charge on the outer surface of the conductor? (c) Use Gauss's Law to find the electric field for radius r < a. (d) Use Gauss's Law to find the electric field for radius a < r < b. (e) Use Gauss's Law to find the electric field for radius r > b. Answer We need to look at this problem in three parts: one, for when the radius ; for when a < r < b, and for when . I. : No charge is enclosed in this case that is, qenc = 0. Therefore, the flux through the Gaussian surface must be zero, and so the electric field = 0 everywhere in this region. II. : Here, the charge enclosed is found by multiplying the total charge Q by the ratio of the volume of charge enclosed by the Gaussian surface to the volume of the entire charged shell: We recall that and as the electric field will be constant everywhere on the spherical Gaussian surface, we can substitute as follows: Therefore, III. : Here, qenc is Q, so we have Again, since the electric field will be constant at every point on the spherical Gaussian surface, we have Which becomes To summarize our findings, here is a plot of the electric field as a function of the radius of the Gaussian surface: Potential Energy, Work, and the Electric Field: The potential energy difference can be defined as the negative of the work done by a conservative force F on an object moved from point A to point B. where dl is a small element of the path from A to B and l is a vector from A to B. Potential Difference: The electric potential difference from point A to point B is the potential energy change per unit charge in moving from A to B. In the case of a uniform field, The Volt and the Electron Volt: The unit of potential difference is the volt (V). 1 V = 1J/C. To say that a car has a 12V battery means that the battery does 12 J of work on every coulomb the moves between its two terminals. The electron volt (eV) is the energy gained by a particle carrying one elementary charge when it moves through a potential difference of one volt. 1eV = 1.602 10-19 J. Calculating Potential Difference: The potential of a point charge. The electric field of a point charge q is given by . Consider two points A and B at distances rA and rB from a positive point charge. The distance between them is rB - rA but we cannot just multiply this distance by the electric field because the field varies with position. Instead we must integrate as follows: What if the points do not lie on the same radial line? The potential difference is independent of path and one path between A and B consists of a radial segment and a circular arc. Since E is perpendicular to the arc, it takes no work to move a charge along the arc. The potential difference therefore arises only from the radial segment. Defining the potential to be zero at some point allows us to speak of the “potential at a point”, meaning the potential difference from the reference point to the point in question. For isolated point charges, a convenient zero is infinitely far from the charge; then the potential at an arbitrary point a distance r from the point q is Potential difference in the field of a line charge We know from before that for field of a line charge. Hence Finding potential differences using superposition: where the ri’s are the distances from each of the charges to the point P. Electric potential is a scalar quantity, so the sum above is a scalar sum, and there is no need to consider angles or vector components. Continuous charge distributions: We can calculate the potential of a continuous charge distribution by considering it to be made up of infinitely many infinitesimal charge elements dq. Each acts like a point charge and therefore contributes to the potential at some point P an amount dV given by where the zero potential is at infinity. The potential at P is the sum of all the contributions dV from all the charge elements. . A charged ring A total charge Q is uniformly distributed over a thin ring of radius a. What is the potential on the axis of the ring? At the center of the ring, A charged disk: A charged disk of radius a carries a total charge Q distributed uniformly over its surface. What is the potential at a point P on the disk’s axis, a distance x from the disk? Divide the disk into charge elements dq. If a ring shaped element has charge dq and radius r, then from above, Then We must relate r and dq. Unwinding the ring gives a strip of area . The surface density is the total charge divided by the disk’s area: . The charge dq on our infinitesimal ring of area is then

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