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Electric Potential Energy versus Electric Potential Calculating the Potential from the Field

Physics 121 - Electricity and Magnetism Lecture 05 -Electric Potential Y&F Chapter 23 Sect. 1-5. Electric Potential Energy versus Electric Potential Calculating the Potential from the Field Potential due to a Point Charge Equipotential Surfaces Calculating the Field from the Potential

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Electric Potential Energy versus Electric Potential Calculating the Potential from the Field

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  1. Physics 121 - Electricity and Magnetism Lecture 05 -Electric Potential Y&F Chapter 23 Sect. 1-5 • Electric Potential Energy versus Electric Potential • Calculating the Potential from the Field • Potential due to a Point Charge • Equipotential Surfaces • Calculating the Field from the Potential • Potentials on, within, and near Conductors • Potential due to a Group of Point Charges • Potential due to a Continuous Charge Distribution • Summary

  2. Initially Q10= 10 C r1= 10 cm Q20= 0 C r2= 20 cm Mechanical analogy: Water pressure Open valve, water flows What determines final water levels? gy = PE/unit mass P2 = rgy2 P1 = rgy1 X Electrostatics: Two spheres, different radii, one with charge Connect wire between spheres, then disconnect it Q1f= ?? Q2f= ?? wire • Are final charges equal? • What determines how charge redistributes itself?

  3. ELECTRIC POTENTIAL Potential Energy due to an electric field per unit (test) charge • Closely related to Electrostatic Potential Energy……but…… • DPE: ~ work done ( = force x displacement) • DV: ~ work done/unit charge ( = field x displacement) • Potential summarizes effect of charge on a distant point without specifying a test charge there (Like field, unlike PE) • Scalar field  Easier to use than E (vector) • Both DPE and DV imply a reference level • Both PE and V are conservative forces/fields, like gravity • Can determine motion of charged particles using: Second Law, F = qE or PE, Work-KE theorem &/or mechanical energy conservation Units, Dimensions: • Potential Energy U: Joules • PotentialV: [U]/[q] Joules/C. = VOLTS • Synonyms for V: both [F][d]/[q], and [q][E][d]/[q] = N.m / C. • Units of field are [V]/[d] = Volts / meter – same as N/C.

  4. Ds I II III IV Reminder: Work Done by a Constant Force 5-1: In the four examples shown in the sketch, a force F acts on an object and does work. In all four cases, the force has the same magnitude and the displacement of the object is to the right and has the same magnitude. Rank the cases in order of the work done by the force on the object, from most positive to the most negative. • I, IV, III, II • II, I, IV, III • III, II, IV, I • I, IV, II, III • III, IV, I, II

  5. Dr I II IV If the force varies in direction and/or magnitude along the path: III Example of a “Path Integral” Result may depend on path Work Done by a Constant Force (a reminder) The work DW done by a constantexternal force on it is the product of: • the magnitude F of the force • the magnitude Δs of the displacement of the point of application of the force • and cos(θ), where θ is the angle between force and displacement vectors:

  6. Recall: Conservative Fields definition • Work done BY THE FIELD on a test charge moving from i to f does notdepend on the path taken. • Work done around any closed path equals zero. (basic definition) POTENTIAL ENERGY DIFFERENCE: Charge q0 moves from i to f along ANY path POTENTIAL DIFFERENCE: (from basic definition) ( Evaluate integrals on ANYpath from i to f ) Potential is potential energy per unit charge Definitions: Electrostatic Potential Energy versus Potential Path Integral

  7. Some distinctions and details • Only differences in electric potential and PE are meaningful: • Relative reference: Choose arbitrary zero reference level for ΔU or ΔV. • Absolute reference: Set Ui = 0 with all charges infinitely far apart • Volt (V) = SI Unit of electric potential • 1 volt = 1 joule per coulomb = 1 J/C • 1 J = 1 VC and 1 J = 1 N m • Electric field units – new name: • 1 N/C = (1 N/C)(1 VC/1 Nm) = 1 V/m • A convenient energy unit: electron volt • 1 eV = work done moving charge e through a 1 volt potential difference = (1.60×10-19 C)(1 J/C) = 1.60×10-19 J • The field depends on a charge distribution elsewhere). • A test charge q0 moved between i and f gains or loses potential energy DU. • DU does not depend on path • DV also does not depend on path and also does not depend on |q0| (test charge). • Use Work-KE theorem to link potential differences to motion

  8. f i E Work and PE : Who/what does positive or negative work? 5-2: In the figure, suppose we exert a force and move the proton from point i to point f in a uniform electric field directed as shown. Which statement of the following is true? A. Electric field does positive work on the proton. Electric potential energy of the proton increases. B. Electric field does negative work on the proton. Electric potential energy of the proton decreases. C. Our force does positive work on the proton. Electric potential energy of the proton increases. D. Our force does positive work on the proton. Electric potential energy of the proton decreases. E. The changes cannot be determined. Hint: which directions pertain to displacement and force?

  9. i E o f Dx To convert potential to/from PE just multiply/divide by q0 EXAMPLE: CHOOSE A SIMPLE PATH THROUGH POINT “O” Displacement i  o is normal to field (path along equipotential) • External agent must do positive work on positive test charge to move it from o  f - units of E can be volts/meter • E field does negative work EXAMPLE: Find change in potential as test charge +q0 moves from point i to f in a uniform field DU and DV depend only on the endpoints ANY PATH from i to f gives same results uniform field What are signs of DU and DV if test charge is negative?

  10. Potential Function for a Point Charge Find potential V(R) a distance R from a point charge q : Positive for q > 0, Negative for q<0 Inversely proportional to r1 NOT r2 Similarly, for potential ENERGY: (use same method but integrate force) Shared PE between q and Q Overall sign depends on both signs Charges are infinitely far apart  choose Vinfinity = 0 (reference level) DU = work done on a test charge as it moves to final location DU = q0DV Field is conservative  choose most convenient path = radial

  11. and DV= 0 Vi > Vf DV= 0 Vfi q DV= 0 CONDUCTORS ARE ALWAYS EQUIPOTENTIALS - Charge on conductors moves to make Einside = 0 - Esurf is perpendicular to surface so DV = 0 along any path on or in a conductor Equi-potential surfaces:Voltage and potential energy are constant; i.e. DV=0, DU=0 No change in potential energy along an equi-potential Zero work is done moving charges along an equi-potential Electric field must be perpendicular to tangent of equipotential Equipotentials are perpendicular to the electric field lines E is the gradient of V

  12. Examples of equipotential surfaces Point charge or outside sphere of charge Uniform Field Dipole Field Equipotentials are planes (evenly spaced) Equipotentials are spheres (not evenly spaced) Equipotentials are not simple shapes

  13. Gradient = spatial rate of change q EXAMPLE: UNIFORM FIELD E – 1 dimension E Ds The field E(r) is the gradient of the potential Component of ds on E produces potential change Component of ds normal to E produces no change Field is normal to equipotential surfaces For path along equipotential, DV = 0

  14. s+ s- L Dx Vi Vf E = 0 Example: Find the potential difference DV across the capacitor, assuming: • s = 1 nanoCoulomb/m2 • Dx = 1 cm & points from negative to positive plate • Uniform field E A positive test charge +q gains potential energy DU = qDV as it moves from - plate to + plate along any path (including external circuit) Potential difference between oppositely charged conductors (parallel plate capacitor) • Equal and opposite surface charges • All charge resides on inner surfaces (opposite charges attract)

  15. FIELD FORCE VECTORS force/unit mass (acceleration) Gravitation force/unit charge (n/C) Electrostatics SCALARS POTENTIAL ENERGY POTENTIAL PE/unit mass (not used often) Gravitation Electrostatics PE/unit charge Fields and forces ~ 1/R2 but Potentials and PEs ~ 1/R1 Comparison of point charge and mass formulas for vector and scalar fields

  16. For q negative V is negative (funnel) r V(r) 1/r r Visualizing the potential function V(r) for a positive point charge (2 D)

  17. r1= 10 cm V10= 90,000 V. Conductors come to same potential Charge redistributes to make it so wire r2= 20 cm V20= 0 V. Initially: Q20= 0 V. Find the final charges: Find the final potential(s): Conductors are always equipotentials Example: Two spheres, different radii, one charged to 90,000 V. Connect wire between spheres – charge moves

  18. Potential inside a hollow conducting shell d c R a b Potential is continuous across surface – field is not V(r) Vinside=Vsurf E(r) Voutside= kq / r Eoutside= kq / r2 Einside=0 r r R R Vc = Vb (shell is an equipotential) = 18,000 Volts on surface R = 10 cm Shell can be any closed surface (sphere or not) Find potential Va at point “a” inside shell Definition: Apply Gauss’ Law: choose GS just inside shell:

  19. Reminder: For the electric field, by superposition, for n point charges Potential due to a group of point charges • Use superposition for n point charges • The sum is an algebraic sum, not a vector sum. • E may be zero where V does not equal to zero. • V may be zero where E does not equal to zero.

  20. Examples: potential due to point charges TWO EQUAL CHARGES – Point P at the midpoint between them +q +q +q -q P P d F and E are zero at P but work would have to be done to move a test charge to P from infinity. Let q = 1 nC, d = 2 m: DIPOLE – Otherwise positioned as above d Let q = 1 nC, d = 2 m: Use Superposition Note: E may be zero where V does not = 0 V may be zero where E does not = 0

  21. Another example: square with charges on corners Find E & V at center point P a -q q d a a P d q -q a + Another example: same as above with all charges positive - Another example: find work done by 12 volt battery in 1 minute as 1 ampere current flows to light lamp i E

  22. q -q q q A B q q q -q q q -q q q -q C D E Electric Field and Electric Potential 5-3: Which of the following figures have V=0 and E=0 at the red point?

  23. 2. Find an expression for dq, the charge in a “small” chunk of the distribution, in terms of l, s, or r Typical challenge: express above in terms of chosen coordinates 3. At point P, dV is the differential contribution to the potential due to a point-like chargedq located in the distribution. Use symmetry. 4. Use “superposition”. Add up (integrate) the contributions over the whole charge distribution, varying the displacement r as needed. Scalar VP. 5. Field E can be gotten from potential by taking the “gradient”: Rate of potential change perpendicular to equipotential Method for finding potential function V at a point P due to a continuous charge distribution 1. Assume V = 0 infinitely far away from charge distribution (finite size)

  24. z P All scalars - no need to worry about direction r z Almost point charge formula y a f dq As z  0, V  kQ/a As a  0 or z  inf, V  point charge x FIND ELECTRIC FIELD USING GRADIENT (along z by symmetry) E  0 as z  0 (for “a” finite) E  point charge formula for z >> a As Before Example 23.11: Potential along Z-axis of a ring of charge Q = charge on the ring l = uniform linear charge density = Q/2pa r = distance from dq to “P” = [a2 + z2]1/2 ds = arc length = adf

  25. Start with • Integrate over the charge distribution • Result Check by differentiating Example: Potential Due to a Charged Rod • A rod of length L located parallel to the x axis has a uniform linear charge density λ. Find the electric potential at a point P located on the y axis a distance d from the origin.

  26. Near line or outside cylinder r > R E is radial. Choose radial integration path if Above is negative for rf > ri with l positive Inside conducting cylinder r < R E is radial. Choose radial integration path if Potential inside is constant and equals surface value Example 23.10: Potential near an infinitely long charged line or charged conducting cylinder

  27. Uniform linear charge density Charge in length dy Potential of point charge Standard integral from tables: Example 23.12: Potential at a symmetry point near a finite line of charge Limiting cases: • Point charge formula for x >> 2a • Example 23.10 formula for near field limit x << 2a

  28. P dA=adfda q r z R a f Double integral Integrate twice: first on azimuthal angle f from 0 to 2p which yields a factor of 2p then on ring radius a from 0 to R x (note: ) “Far field” (z>>R): disc looks like point charge Use Anti-derivative: “Near field” (z<<R): disc looks like infinite sheet of charge Example: Potential on the symmetry axis of a charged disk Q = charge on disk whose radius = R. Uniform surface charge density s = Q/4pR2 Disc is a set of rings, each of them da wide in radius For one of the rings:

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