Lecture 4 Work, Electric Potential and Potential Energy Ch. 25 - PowerPoint PPT Presentation

lecture 4 work electric potential and potential energy ch 25 n.
Download
Skip this Video
Loading SlideShow in 5 Seconds..
Lecture 4 Work, Electric Potential and Potential Energy Ch. 25 PowerPoint Presentation
Download Presentation
Lecture 4 Work, Electric Potential and Potential Energy Ch. 25

play fullscreen
1 / 44
Lecture 4 Work, Electric Potential and Potential Energy Ch. 25
690 Views
Download Presentation
andren
Download Presentation

Lecture 4 Work, Electric Potential and Potential Energy Ch. 25

- - - - - - - - - - - - - - - - - - - - - - - - - - - E N D - - - - - - - - - - - - - - - - - - - - - - - - - - -
Presentation Transcript

  1. Lecture 4 Work, Electric Potential and Potential Energy Ch. 25 • Topics • Work, electric potential energy and electric potential • Calculation of potential from field • Potential from a point charge • Potential due to a group of point charges, electric dipole • Potential due to continuous charged distributions • Calculating the electric field from a potential • Electric potential energy from a system of point charges • Equipotential Surface • Potential of a charged isolated conductor • Demos • Teflon and silk • Charge Tester, non-spherical conductor, compare charge density at different radii. • Elmo • Potential in the center of four charges • Potential of a electric dipole • Polling

  2. Work, Potential Energy and Electric potential • The electric force is mathematically the same as gravity so it too must be a conservative force. We want to show that the work done is independent of the path and only depends on the endpoints. Then the force is said to be a conservative force. • First start with work Work done by the electric force = • Then we will find it useful to define a potential energy as is the case for gravity. • And the electric potential

  3. b P2 P3 c a E P1 Lets start with a uniform electric field and find the work done for a positive test charge.

  4. b P2 P3 F c a E P1 Find work done along path W12 for a positive test charge

  5. F b P2 P3 c a E P1 Find Work along path W23

  6. W12 + W23 = 0 + qEb =qEb Compare this work done along path W13

  7. Work done along path W13 b P2 P3  c a  F P1

  8. Conclusion • Work done along path W12 + W23 = W13. • Work is independent of the particular path. • Although we proved it for a uniform field, it is true for any field that is a only a function of r and is along r. • It only depends on the end points i and f. • This means we can define a function at every point in space and when we take the difference of that function between any two points, it is equal to the negative of the work done.

  9. b P2 P3 c a  F P1 When we go from P1 to P3 we evaluate the Work function at P3 and subtract the value at P1 and then the a difference equals the negative of the work done in going form P1 to P3. This function is called the potential energy function

  10. Example of finding the Potential Energy Function U in a Uniform Field E E d b a What is the electric potential difference for a unit positive charge moving in an uniform electric field from a to b? If we set the origin at xb = 0, and measure from b to a, then Ub=0 and the potential energy function is U=qEd This is analogy with gravitation where we U =mgh.

  11. Now define the Electric Potential Difference V which does not depend on charge. • The potential difference is the negative of the work done per unit charge by an electric field on a positive unit charge when it moves from one point to another.

  12. Find the potential difference V for a uniform electric field For a battery of potential difference of 9 volts you would say that the positive terminal is 9 volts above the negative terminal.

  13. Note relationship between potential and electric field • V is a scalar not a vector. Simplifies solving problems. • We are free to choose V to be 0 at any location. Normally V is chosen to be 0 at the negative terminal of a battery or 0 at infinity for a point charge.

  14. Example for a battery in a circuit • In a 9 volt battery, typically used in IC circuits, the positive terminal has a potential 9 v higher than the negative terminal. If one micro-Coulomb of positive charge flows through an external circuit from the positive to negative terminal, how much has its potential energy been changed? q

  15. Generalize concept of electric potential energy and potential difference for any electric field

  16. = - Work done by the electric force = y x (independent of path, ds) Therefore, electric force is a conservative force.

  17. Find the electric potential when moving from one point to another in a field due to a point charge?

  18. Potential of a point charge at a distance R Replace R with r eqn 25-26

  19. Electric potential for a positive point charge • V is a scalar • V is positive for positive charges, negative for negative charges. • r is always positive. • For many point charges, the potential at a point in space is the simple algebraic sum (Not a vector sum)

  20. Electric potential due to a positive point charge Hydrogen atom. • What is the electric potential at a distance of 0.529 A from the proton? 1A= 10-10 m r = 0.529 A • What is the electric potential energy of the electron at that point? U = qV= (-1.6 x 10-19 C) (27.2 V) = - 43.52 x 10-19 J or - 27.2 eV where eV stands for electron volt. Note that the total energy E of the electron in the ground state of hydrogen is - 13.6 eV Also U= 2E = -27.2 eV. This agrees with above formula.

  21. What is the electric potential due to several point charges? For many point charges, the potential at a point in space is the simple algebraic sum (Not a vector sum) y q2 q1 r2 r1 q3 r3 x

  22. Four Point charges

  23. Two point charges that are opposite and equal What is the potential due to a dipole?

  24. Potential for a Continuous Distribution of Charge Point charge For an element of charge Integrate V

  25. Chaper 24 Problem 22. With V = 0 at infinity, what is the electric potential at P, the center of curvature of the uniformly charged nonconducting rod?

  26. Chapter 24 Problem 26. What is the magnitude of the net electric potential at the center? 1. A thin rod of charge -3.0 µC that forms a full circle of radius 6.0 cm2. A second thin rod of charge 2.0 µC that forms a circular arc of radius 4.0 cm, subtending an angle of 90° about the center of the full circle3. An electric dipole with a dipole moment that is perpendicular to a radial line andthat has magnitude 1.28 multiplied by 10-21 C·m

  27. Figure 24-44 shows a thin plastic rod of length L and uniform positive charge Q lying on an x axis. With V = 0 at infinity, find the electric potential at point P1 on the axis, at distance d from one end of the rod.

  28. Potential due to a ring of charge • Direct integration. Since V is a scalar, it is easier to evaluate V than E. • Find V on the axis of a ring of total charge Q. Use the formula for a point charge, but replace q with elemental charge dq and integrate. Point charge For an element of charge r is a constant as we integrate. V This is simpler than finding E because V is not a vector.

  29. Potential due to a line charge We know that for an element of charge dq the potential is For the line charge let the charge density be l. Then dq=ldx Now, we can find the total potential V produced by the rod at point P by integrating along the length of the rod from x=0 to x=L

  30. A new method to find E if the potential is known.If we know V, how do we find E? So the x component of E is the derivative of V with respect to x, etc. • If V = a constant, then Ex = 0. The lines or surfaces on which V remains constant are called equipotential lines or surfaces. • See example on next slide

  31. Now find the electric field at point P1 on the axis, at distance d from one end of the rod. Find the x and y components Ex and Ey.

  32. Equipotential Surfaces • Three examples • What is the equipotential surface and equipotential volume for an arbitrary shaped charged conductor? • See physlet 9.3.2 Which equipotential surfaces fit the field lines?

  33. x Blue lines are the electric field lines Orange dotted lines represent the equipotential surfaces a) Uniform E field V = constant in y and z directions c) Electric Dipole (ellipsoidal concentric shells) • Point charge (concentric shells)

  34. Electric Potential Energy U of a system of charges How much work is required to set up the arrangement of Figure 24-46 if q = 3.20 pC, a = 54.0 cm, and the particles are initially infinitely far apart and at rest? q2 W = U q1 q3 q4

  35. Dielectric Breakdown: Application of Gauss’s Law If the electric field in a gas exceeds a certain value, the gas breaks down and you get a spark or lightning bolt if the gas is air. In dry air at STP, you get a spark when V = constant on surface of conductor Radius r2 r1 1 2

  36. This explains why: • Sharp points on conductors have the highest electric fields and cause corona discharge or sparks. • Pick up the most charge with charge tester from the pointy regions of the non-spherical conductor. • Use non-spherical metal conductor charged with teflon rod. Show variation of charge across surface with charge tester. Radius R V = constant on surface of conductor 1 Cloud 2 + + + + Van de Graaff - - - -

  37. How does a conductor shield the interior from an exterior electric field? • Start out with a uniform electric field with no excess charge on conductor. Electrons on surface of conductor adjust so that: 1. E=0 inside conductor 2. Electric field lines are perpendicular to the surface. Suppose they weren’t? 3. Does E = just outside the conductor 4. Is s uniform over the surface? 5. Is the surface an equipotential? 6. If the surface had an excess charge, how would your answers change?

  38. What is the electric potential of a uniformly charged circular disk? We can treat the disk as a set of ring charges. The ring of radius R’ and thickness dR’ has an area of 2pR’dR’ and it’s charge is dq = sdA = s(2pR’)dR’ where s=Q/(pR2), the surface charge density. The potential dV at point P due to the charge dq on this ring given by q Integrating R’ from R’=0 to R’=R

  39. Chapter 24 Problem 19 The ammonia molecule NH3 has a permanent electric dipole moment equal to 1.31 D, where 1 D = 1 debye unit = 3.34 multiplied by 10-30 C·m. Calculate the electric potential due to an ammonia molecule at a point 44.0 nm away along the axis of the dipole. (Set V = 0 at infinity.)

  40. Chapter 24 Problem 55 Two metal spheres, each of radius 1.0 cm, have a center-to-center separation of 2.2 m. Sphere 1 has charge +2.0 multiplied by 10-8 C. Sphere 2 has charge of -3.8 multiplied by 10-8 C. Assume that the separation is large enough for us to assume that the charge on each sphere is uniformly distributed (the spheres do not affect each other). Take V = 0 at infinity. (a) Calculate the potential at the point halfway between the centers. (b) Calculate the potential on the surface of sphere 1. (c) Calculate the potential on the surface of sphere 2.

  41. Chapter 24 Problem 57 A metal sphere of radius 11 cm has a net charge of 2.0 multiplied by 10-8 C. (a) What is the electric field at the sphere's surface? (b) If V = 0 at infinity, what is the electric potential at the sphere's surface? (c) At what distance from the sphere's surface has the electric potential decreased by 500 V?