A charged particle within a field-rich environment can be subjected to multiple forces based on the prevailing conditions. The primary forces acting on a charged particle are delineated below:
This force arises from the interaction between two electric charges. Coulomb's law quantifies this force, establishing it as directly proportional to the product of the charges' magnitudes and inversely proportional to the square of the separation distance:
\[ F = k_e \frac{|q_1 q_2|}{r^2} \]
wherein:
The force is attractive for charges of opposite signs and repulsive for like charges.
All objects possessing mass, including charged particles, are subject to gravitational force, as described by Newton's law of universal gravitation:
\[ F_g = \frac{G m_1 m_2}{r^2} \]
where:
It is noteworthy that the gravitational force exerted on charged particles is exceedingly weak in comparison to other forces, such as the electrostatic force, due to the diminutive masses of subatomic particles relative to their charges.
A charged particle in motion within a magnetic field experiences a magnetic force. This interaction is governed by the Lorentz force law, which indicates that the magnetic force is proportional to the particle's charge, velocity, and the magnetic field strength:
\[ F_B = q \vec{v} \times \vec{B} \]
with:
The resultant magnetic force is orthogonal to both the particle's velocity and the magnetic field.
The combined force experienced by a charged particle subjected to both electric and magnetic fields is termed the Lorentz force. It is the summation of the electrostatic and magnetic forces:
\[ \vec{F} = q(\vec{E} + \vec{v} \times \vec{B}) \]
where:
The Lorentz force dictates the behavior of charged particles under the influence of electric and magnetic fields.
When a charged particle follows a circular trajectory due to a magnetic field, the magnetic force serves as the centripetal force maintaining this motion. The centripetal force is calculated as:
\[ F_c = \frac{m v^2}{r} \]
where:
A charged particle situated within an external electric field experiences an electric force defined by:
\[ F_E = qE \]
where:
This force drives the acceleration of a positive charge in the direction of the electric field and a negative charge in the opposite direction.
In summary, the forces that can impact a charged particle include: