Current density is a vector quantity that describes the current per unit area flowing through a conductor. It provides a more detailed description of how current is distributed within a material and is essential for understanding current flow in conductors of varying cross-sectional areas.
Definition of Current Density
$$\vec{J} = \frac{I}{A} \hat{n}$$
Current density is defined as the current per unit area, where the direction is specified by the unit vector \(\hat{n}\) in the direction of current flow.
Units: A/m² (amperes per square meter)
Direction: Same as conventional current direction
Vector quantity: Has both magnitude and direction
Microscopic description: Provides detailed current distribution
Current density vector showing magnitude and direction of current flow per unit area.
Relationship to Current
$$I = \int \vec{J} \cdot d\vec{A}$$
The total current through a surface is the flux of current density through that surface. For uniform current density, this simplifies to:
$$I = JA \cos\theta$$
Where:
\(I\) = total current
\(J\) = current density magnitude
\(A\) = cross-sectional area
\(\theta\) = angle between current density and area normal
Perpendicular flow: When \(\theta = 0°\), \(I = JA\)
Parallel flow: When \(\theta = 90°\), \(I = 0\)
Microscopic Expression
$$\vec{J} = nq\vec{v}_d$$
Current density can also be expressed in terms of the microscopic properties of the conductor.
Where:
\(n\) = number density of charge carriers
\(q\) = charge of each carrier
\(\vec{v}_d\) = drift velocity vector
For electrons: \(q = -e\) (negative charge)
For holes: \(q = +e\) (positive charge)
Direction: Opposite to electron drift velocity
Memory Trick: NEVADA for Current Density
Remember the current density formula using NEVADA:
NE = \(ne\) (number density × elementary charge)
V = drift velocity (\(v_d\))
A = area (related to current density)
D = density (current density \(J\))
A = area again (cross-sectional area)
So: \(ne \times v_d = J\) (current density)
And: \(J \times A = I\) (total current)
This helps you remember that \(nev_d = J\), which is the microscopic expression for current density!
Current Density in Different Geometries
Uniform Current Density
When current density is constant across the cross-section:
$$J = \frac{I}{A} = \text{constant}$$
Non-Uniform Current Density
When current density varies across the cross-section, the total current is:
$$I = \int J(r) \, dA$$
Example: Radial Current Density
Problem: A cylindrical conductor has current density that varies with radius as \(J(r) = J_0(1 - r/R)\), where \(R\) is the radius. Find the total current.
Solution:
Area element: \(dA = 2\pi r \, dr\)
Current element: \(dI = J(r) \, dA = J_0(1 - r/R) \cdot 2\pi r \, dr\)
Total current: \(I = \int_0^R J_0(1 - r/R) \cdot 2\pi r \, dr\)
Example 3: Current from Non-Uniform Current Density
Problem: A wire has current density that varies as \(J(r) = J_0 r/R\), where \(R\) is the radius. If \(J_0 = 2.0 \times 10^6 \text{ A/m}^2\) and \(R = 1.0 \text{ mm}\), find the total current.
Solution:
Current element: \(dI = J(r) \cdot 2\pi r \, dr = J_0 \frac{r}{R} \cdot 2\pi r \, dr\)
Total current: \(I = 2\pi J_0 \int_0^R \frac{r^2}{R} \, dr\)
Problem: Two wires are connected in parallel. Wire A has radius 1.0 mm and carries 3.0 A. Wire B has radius 2.0 mm and carries 5.0 A. Which wire has higher current density?