Notes: Potential (V)

Relationship to E
  • only depends on source charges (not test charges)
  • V can be determined by E
  • Ex: constant E → ΔV = Ex Δx
Charge distributions
  • Point charge → V = ke q / r
  • Flat uniform surface of charge → V = -2 π ke σ d
  • Uniform hollow sphere → V = ke Q / r (outside), ke Q / R (inside)
  • Equipotentials for each distribution
Reminders
  • V is high near + charge, low near -
  • E points from high V to low V

Example: 2 charges (V vs. Ex)

V
  • VLeft = 9×109 N m2/C2 * 1.0×10-9C * / .005m = 1800V
  • VRight = ?
  • V = 3600V
E
  • ELeft = 9×109 N m2/C2 * 1.0×10-9C * / (0.005m)2 = 360000N/C to right
  • ERight = ?
  • E = 0
+ and -
  • Imagine instead we had a +1.0nC charge on the left, and a -1.0nC charge on the right.
  • What will V be?
  • What will E be?

Example: Particle collision

NOTE
  • acceleration is NOT constant (draw E field of a single electron)
  • → using Newton's 2nd law will not be feasible
Solution
  • Given: ri = 1.0m, m = 9.1×10-31kg, vi = 1.0×105m/s
  • Context: vf = 0
  • Looking for rf
  • Principles: Electric potential of point charge, conservation of energy, kinetic energy
  • V = ke q / r, PE = q V
Pause
  • Will KEi be positive or negative? (ALWAYS positive)
  • Will PEi be positive or negative? (positive: q < 0, V < 0, PE > 0)
  • As electrons approach each other, will PE increase or decrease? (increase)
  • What must happen, then, to KE?
Solution (ctd)
  • KEi = 9e-21J, PEi = 2.3e-28J (ignore)
  • PEf = 9e-21J → rf = 2.6e-8m