Theme D — Fields
D.2.7 Electric Potential — IB Physics HL Revision Notes & Topical Questions
5 min read 10 parts Lesson 22 of 39 1 quiz
Curriculum Equation Key قوانين الرقم الهيدروجيني والاتزان الأيوني - pH & Acid-Base Equilibrium FormulasFast Exam Solution
pH = -log[H⁺] | pOH = -log[OH⁻] | pH + pOH = 14 | [H⁺][OH⁻] = 10⁻¹⁴
Word Equation & Conditions: الرقم الهيدروجيني = -لوغاريتم تركيز أيون الهيدروجين | pH + pOH = 14
Location & Specifications: الاتزان الأيوني، كيمياء 3 ثانوي، التحصيلي، و AP Chemistry.
Lesson summary
D.2.7 Electric Potential — IB PHYSICS HL notes: Define electric potential, use V = kQ/r for point charges and spheres, and add potentials from several charges.Electric potential — the work done per unit charge in taking a small positive test charge from infinity to a defined poin…
- Depends on
- Conducting sphere
- Inside a charged sphere
- Positive charge
- Negative charge
- Field lines
Part 1 of 8Definition
Electric potential
- Electric potential the work done per unit charge in taking a small positive test charge from infinity to a defined point
Unit
- Unit joule per coulomb, J C−1, which is the volt
Scalar
- Scalar it has no direction but a sign matching the charge
Reference
- Reference zero at infinity, as for gravitational potential
Depends on
- Depends on the size of the charge and the distance from it
Part 2 of 8Potential of a point charge
Equation
- V = kQ/r = Q/(4πε0r)
Q
Q the charge producing the potential, with its sign
r
r the distance from the centre of the point charge
Conducting sphere
- Conducting sphere the same equation applies with the charge treated as concentrated at the centre
Inside a charged sphere
- Inside a charged sphere the potential is constant
Sign
- V has the sign of Q, unlike gravitational potential which is always negative
Part 3 of 8Positive and negative charges
Positive charge
- V is positive, rises as a test charge moves closer and falls with distance
- Energy must be supplied to push a positive test charge closer
Negative charge
- V is negative, falls as a test charge moves closer and rises towards zero with distance
- Energy is released as a positive test charge moves closer
Field lines
- Field lines potential always decreases in the direction of the field lines
Free charges
- Free charges a free positive charge accelerates towards lower potential and a free negative charge towards higher potential
Part 4 of 8Combining potentials
Superposition
- V = kQ1/r1 + kQ2/r2 + …, adding algebraically with signs
Equal charges
- Equal charges a point equidistant from two equal positive charges has double the potential of one
Dipole
- Dipole at the midpoint V = 0 although the field is not zero, because fields add as vectors
Part 5 of 8Potential difference and work
1Potential difference
- ΔV = Vf − Vi
2Point charge
- ΔV = kQ(1/rf − 1/ri)
3Work by an external agent
- W = qΔV, where q is the charge being moved
4Field
- Field it does the negative of this work
Part 6 of 8Potential and field compared
| Quantity | Electric potential | Electric field strength |
|---|---|---|
| Type | Scalar | Vector |
| Unit | V or J C−1 | V m−1 or N C−1 |
| Point charge | kQ/r, falls as 1/r | kQ/r2, falls as 1/r2 |
| Information | Energy per unit charge | Force per unit charge |
Part 7 of 8More from the specification
1Zero reference ground on Earth
- Zero reference ground on Earth physically connecting conducting shells to the planet Earth establishes a stable zero volt reference electric potential.
2Electric Potential and Equipotential Surfaces
- An equipotential surface connects points of identical electric potential;
- between parallel plates, equipotentials form parallel planes perpendicular to electric field lines, requiring zero work to move a charge across the surface.
3Potential Gradient and Field Strength
- The magnitude of the electric field strength E equals the negative gradient of the electric potential graph with respect to distance (E = -dV/dr), directed toward regions of lower potential.
4Electrostatic vs Magnetic Forces
- While electric forces act on charges parallel to field lines between charged plates, moving charges in a magnetic field experience Lorentz forces perpendicular to both velocity and magnetic field lines.
- (electric current)
5Electric Potential and Equipotential Surfaces
- An equipotential surface connects points of identical electric potential;
- between parallel plates, equipotentials form parallel planes perpendicular to electric field lines, requiring zero work to move a charge across the surface.
6Potential Gradient and Field Strength
- The magnitude of the electric field strength E equals the negative gradient of the electric potential graph with respect to distance (E = -dV/dr), directed toward regions of lower potential.
7Electrostatic vs Magnetic Forces
- While electric forces act on charges parallel to field lines between charged plates, moving charges in a magnetic field experience Lorentz forces perpendicular to both velocity and magnetic field lines.
- (electric current)
8Relative permittivity
- Ratio of the permittivity of a material to that of free space.
9Equipotential
- A surface of constant potential
10Parallel
- Components on separate branches, each with the full e.m.f.
11Permittivity
- A property of a medium affecting the electric force within it.
12Current
- Flow of electrons in a circuit.
13Uniform
- Same density throughout, so the weight acts at the centre.
14Density
- Mass per unit volume.
15Magnetic field
- Area around a magnet where its effects can be detected.
16Equipotential line
- A line joining points of equal gravitational potential.
Part 8 of 8More from the specification
- W = mgWhat the symbols mean: W = weight (N) · m = mass (kg) · g = gravitational field strength (9.81 N kg−1 on Earth)
Key terms
| Term | Meaning |
|---|---|
| Electric potential | The work done per unit charge in taking a small positive test charge from infinity to the point. |
| Volt | One joule per coulomb. |
| Potential difference | The work done per unit charge moving a charge between two points. |
| Scalar | A quantity with magnitude but no direction. |
Avoid these mistakes
1
Treating potential as a vector and adding with directions.
2
Dropping the sign of Q in V = kQ/r.
3
Confusing potential (J C−1) with potential energy (J).
4
Believing V = 0 means E = 0, or the reverse.
5
Using r from the surface rather than from the centre of a charged sphere.
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