**Current density**represents the current flowing per unit area of cross-section at a point. To relate current, a microscopic quantity, to the microscopic motion of the charges, let's examine a conductor of cross-sectional area A, as shown in given figure.

A microscopic picture of current flowing in a conductor

The total current through a surface can be written as

where is the current density (the SI unit of current density are A/m

^{2}). If q is the charge of each carrier, and n is the number of charge carriers per unit volume, the total amount of charge in this section Q = q(nAx). Suppose that the charge carriers move with a speed v

_{d}. then the displacement in a time interval t will be x = v

_{d}t, which implies

The speed v

_{d}at which the charge carriers are moving is known as the drift speed. Physically, v

_{d}is the average speed of the charge carriers inside a conductor when an external electric field is applied. Actually an electron inside the conductor does not travel in a straight line; instead, its path is rather erratic as shown.

Motion of an electron in a conductor

From the above equations, the current density can be written as

= nq

_{d}

Thus, we see that and

_{d}point in the same direction for positive charge carriers, in opposite directions for negative charge carriers.

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