Free electrons entering a magnetic field at a right angle will follow a circular path due to the Lorentz force law, which states that the force experienced by the electron is perpendicular to both its velocity and the magnetic field direction. This force is constant in magnitude and direction, leading to a circular trajectory as long as the electron's speed is not relativistic. However, the path cannot be a complete circle within a static homogeneous field, as electrons must exit the field after entering. While more complex relativistic effects exist, the circular motion remains a valid approximation for non-relativistic speeds. Understanding this behavior is crucial for applications in electromagnetism and particle physics.