In a solid cylindrical resistor like copper at room temperature, the drift velocity of conduction electrons is directly proportional to the current flowing through the conductor. The thermal velocity of these electrons is influenced by temperature, with a formula of sqrt(3kT/m) indicating it reaches around 10^5 m/s at room temperature. While the drift velocity and current are linked through the equation I = vnqA, where n is electron concentration, q is charge, and A is cross-sectional area, the thermal velocity remains largely unaffected by current changes. The current density can be expressed as J = vnq, establishing a relationship between particle flux and electron concentration. Overall, the interplay between current, drift velocity, and thermal velocity is crucial for understanding electron behavior in conductors.