The charge density formula in its volume form is : the charge in a region divided by the volume of that region, in coulombs per cubic metre. When charge lies on a surface or along a line instead, you switch to or .
Which one a question wants depends on the shape. A solid ball of charge needs ρ, a metal plate needs σ, and a long thin wire needs λ. This page sets out all three side by side, works an example of each, and shows how they feed into the field formulas you use in Class 12 and AP Physics 2.
Quick facts
Volume
, unit C/m³Surface
, unit C/m²Line
, unit C/mDimensional formula of ρ
[M⁰ L⁻³ T¹ I¹]Type
Scalar, positive or negativeCarrier form
for n carriers per m³
Choosing the right charge density formula
| Kind | Symbol and formula | SI unit | Typical object |
|---|---|---|---|
| Volume | C/m³ | Uniformly charged sphere or cylinder | |
| Surface | C/m² | Conducting plate, spherical shell | |
| Line | C/m | Thin rod, wire, ring |
Ask yourself how many dimensions the charge is spread over. Three dimensions means ρ, two means σ, one means λ. Each is an average if the charge is uneven; the point value uses a small element, such as .
Worked examples for each type
Example 1: a charged ball
A solid insulating sphere of radius 5.0 cm holds 2.0 μC spread through its volume. Find ρ.
V = (4/3)π(0.050)³ = 5.24 × 10⁻⁴ m³.
Example 2: a thin rod
A 2.0 m rod carries 6.0 nC evenly along its length. Find λ.
Each metre of the rod carries 3 nC.
Example 3: a disc
A disc of radius 0.10 m holds 3.14 nC on one face. Find σ.
A = π(0.10)² = 0.0314 m².
Volume formulas and conversions
| Item | Value |
|---|---|
| Sphere of radius R | |
| Cylinder of radius r, length L | |
| One cubic centimetre | a millionth of a cubic metre (10⁻⁶ m³) |
| One litre | a thousandth of a cubic metre (10⁻³ m³) |
| 1 μC/cm³ | 1 C/m³ |
The last row surprises students: the 10⁻⁶ in the microcoulomb cancels the 10⁻⁶ in the cubic centimetre. Always write the powers of ten out before cancelling.
Charge density and the field inside a charged sphere
Inside a uniformly charged ball, only the charge within radius r counts. That charge is , and Gauss's law gives
So the field grows in a straight line from zero at the centre to its largest value at the surface, then falls as 1/r² outside. Field results for sheets and lines use the surface and linear densities, and are listed on the electric field page.
Charge density of carriers in a metal
In current electricity, the same idea describes the mobile electrons. If a metal has n free electrons per cubic metre, their charge density is . For copper, n ≈ 8.5 × 10²⁸ m⁻³, so the mobile charge is about 1.4 × 10¹⁰ C/m³, cancelled exactly by the positive ions. That huge reservoir is why a small drift velocity is enough to carry everyday currents, through .
Avoiding common errors
- Using a surface area when the charge fills a volume, or the other way round.
- Cubing the diameter instead of the radius.
- Dropping the negative sign on electron charge densities.
- Mixing up the three Greek letters: λ for line, σ for surface, ρ for volume.
The detailed page for the volume form is volume charge density. The electricity formulas hub lists every page in this chapter.
Frequently asked questions
What is the formula for charge density?
For a volume, ρ = q / V. For a surface, σ = q / A. For a line, λ = q / L.
Which units go with each kind of charge density?
Volume charge density is in C/m³, surface charge density in C/m² and linear charge density in C/m.
Is charge density a scalar?
Yes. It has no direction, only a size and a sign.
What is the dimensional formula of volume charge density?
Charge is [I T] and volume is [L³], so ρ works out to [M⁰ L⁻³ T¹ I¹].
How is charge density different from charge?
Charge is the total amount in coulombs. Charge density says how that amount is spread, per metre, square metre or cubic metre.