To understand the velocity of charge carriers in a metal under normal conditions when the current is about 1 ampere, we must explore the concept of drift velocity in conductors.
In a conductor, charge carriers (usually electrons) experience a small and average velocity known as the drift velocity due to the presence of an electric field. The drift velocity of electrons in a metallic conductor with current is given by the formula:
v_d = \frac{I}{nAe}, where:
In good conductors (like metals), despite a high density of charge carriers, the drift velocity is typically very small because of the small acceleration imparted due to the electric field.
For common metal conductors, this drift velocity is indeed very tiny, often about a fraction of a millimeter per second. This is due to the large number of electrons available per unit volume of the conductor and the relatively modest current value of 1 A compared to the massive number of available carriers.
Therefore, given the options, the correct answer is that the velocity of charge carriers is a fraction of mm/sec.
Let's briefly evaluate why the other options are incorrect:
In conclusion, the drift velocity of the order of a fraction of mm/sec aligns well with typical values observed for metals carrying a current of about 1 ampere.