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Unit 3: Electric Potential

Trading vectors for one number that remembers the work it takes to build a charge configuration, and a field you can recover from a potential's slope.

9 topics · 33 questions

Each topic is a path, not a menu: work down it in order and every question builds on the one above. Click any of them to watch the answer draw itself.

Electric Potential Energy

  1. How it worksHow does the work done assembling two point charges become the electric potential energy of the pair?
  2. Worked exampleFind the potential energy of a +4 microcoulomb and a -2 microcoulomb charge separated by 30 cm.
  3. Common mistakeWhy isn't electric potential energy something a single, isolated charge can be said to have on its own?
  4. Going furtherWhat happens to the potential energy of two charges as they're pulled apart to an infinite separation?
  5. Worked exampleFind the total potential energy of three +2 nC point charges placed at the corners of an equilateral triangle of side 10 cm.
Your turn1 of 2
Find the electric potential energy of a +7 microC charge and a -6 microC charge separated by 47 cm. Use k = 8.99x109 N m2/C2.

Electric Potential and Voltage

  1. How it worksHow does moving a charge against a field raise its potential the way lifting a mass raises its potential energy?
  2. Worked exampleFind the potential difference needed to give a proton 2 times 10 to the -16 joules of kinetic energy from rest.
  3. Common mistakeWhy doesn't a higher electric potential at a point automatically mean a stronger field is sitting there?
  4. Ties togetherHow does electric potential play the same role for charge that height plays for mass in gravity?
Your turn1 of 2
Find the potential difference needed to give a proton 7 times 10−16 joules of kinetic energy, starting from rest. Use the proton's charge e = 1.602x10−19 C.

The Potential of a Point Charge

  1. How it worksHow does integrating the electric field along a path from infinity give the potential of a point charge?
  2. Worked exampleFind the electric potential 50 cm from a point charge of +8 nanocoulombs.
  3. Going furtherWhat happens to the potential from several point charges as a test charge is moved in from far away?
Your turn1 of 2
Find the electric potential 68 cm from a point charge of +35 nC. Use k = 8.99x109 N m2/C2.

Potential of a Continuous Charge Distribution by Integration

  1. How it worksHow does integrating dq over r turn a whole charged object into a single potential value at one point?
  2. Worked exampleFind the potential on the axis of a charged ring of radius 6 cm and charge 5 nC, 8 cm from its center.
  3. Going furtherWhat happens to a charged ring's potential as the observation point moves far beyond the ring's own radius?
Your turn1 of 2
Find the electric potential on the axis of a charged ring of radius 8 cm and charge 6 nC, 19 cm from its center. Use k = 8.99x109 N m2/C2.

Equipotential Surfaces

  1. How it worksHow do equipotential surfaces always end up perpendicular to the field lines that cross through them?
  2. Common mistakeWhy isn't it possible for two genuinely different equipotential surfaces to touch or cross each other?
  3. How it worksWalk me through sketching the equipotential surfaces surrounding a single, isolated point charge.
  4. Going furtherWhat do the equipotential surfaces look like around two equal and opposite point charges?
  5. Common mistakeWhy doesn't moving a charge along an equipotential surface ever change that charge's kinetic energy?
Your turn1 of 2
Does every point in space sit on exactly one equipotential surface, so that surfaces at two different potential values can never touch or cross?

Finding the Electric Field from the Potential

  1. How it worksHow does taking the negative slope of the potential in a direction give the field component in that direction?
  2. Worked exampleFind the electric field between two plates 2 cm apart held at a potential difference of 500 volts.
  3. Common mistakeWhy doesn't a region of high potential have to be a region where the electric field is especially strong?
  4. Going furtherWhat happens to the electric field wherever the potential is flat, with no change from point to point?
Your turn1 of 2
Find the electric field between two plates 7 cm apart held at a potential difference of 667 volts.

Why a Whole Conductor Sits at One Potential

  1. How it worksHow does the zero field inside a conductor force its entire volume to share a single potential value?
  2. Common mistakeWhy doesn't a conductor's irregular shape create different potentials at different points on its own surface?
  3. Ties togetherHow does a conductor being one equipotential connect back to the field vanishing throughout its interior?
Your turn1 of 2
A charged conducting sphere of radius 15 cm carries charge 13 nC. Find the electric potential at its surface, which also equals the potential everywhere inside it. Use k = 8.99x109 N m2/C2.

Energy in Electron Volts

  1. How it worksHow does accelerating a charge through a one-volt potential difference define the electron volt as a unit?
  2. Worked exampleFind the kinetic energy in electron volts of an electron accelerated through a potential difference of 4000 volts.
  3. Going furtherWhat happens to the size of the natural energy unit when you're describing a proton instead of an electron?
Your turn1 of 2
Find the kinetic energy, in electron volts, of an electron accelerated through a potential difference of 6995 volts.

Applications of Electrostatics

  1. How it worksHow does a moving belt keep piling charge onto a hollow metal sphere until sparks fly off its surface?
  2. How it worksWalk me through how a lightning rod protects a building by controlling where the field grows strongest.
  3. Ties togetherHow does charge piling up at sharp points explain both a lightning rod and a Van de Graaff generator?
Your turn1 of 2
A Van de Graaff generator uses a moving belt to carry charge onto a large hollow metal dome. Where does essentially all of that charge end up once it reaches the dome?