The force felt by a charged particle in an electric field is described by:
F = qE
The force felt by a charged particle in an electric field is equal to the charge of the particle, q, multiplied by the electric field value, E.
The direction of the force on a positive charge is in the same direction as the electric field; the direction of the force on a negative charge is opposite the electric field.
A charged particle in an electric field can have electrical potential energy.
Electric Potential: Potential energy provided by an electric field per unit charge; also called voltage.
Electric potential is a scalar quantity. The units of electric potential are volts. 1 volt = 1 J/C.
Equipotential Lines: Lines that illustrate every point at which a charged particle would experience a given potential.
On the left, the electric field points away from the positive charge. At any particular distance away from the positive charge, you would find an equipotential line that circles the charge.
On the right is a uniform electric field. The equipotential lines are drawn perpendicular to the electric field lines.
If you take two metal plates, charge one positive and one negative, and then put them parallel to each other, you create a uniform electric field in the middle.
The electric field between the plates has a magnitude of
V is the voltage difference between the plates.
d is the distance between the plates.
Charged parallel plates can be used to make a capacitor, a charge-storage device.
The space between the plates prevents any charges from jumping from one plate to the other while the capacitor is charged.
The amount of charge that each plate can hold is described by the following equation:
Q = CV
Q is the charge on each plate
C is called the “capacitance,”
The capacitance is a property of the capacitor you are working with, and it is determined primarily by the size of the plates and the distance between the plates, as well as by the material that fills the space between the plates.
The units of capacitance are farads, abbreviated F; 1 coulomb/volt = 1 farad.V is the voltage across the plates.
A is the area of each plate, and d is the distance between the plates (in m).
The term ε0 (pronounced “epsilon-naught”) is called the “permittivity of free space.” TThe value of ε0 is 8.84 × 10–12 C/V·m.
Q is the charge of your point charge
ε0 is the permittivity of free space
r is the distance away from the point charge
Second, the electric potential at some distance away from a point charge:
And third, the force that one point charge exerts on another point charge:
Q1 is the charge of one of the point charges, and Q2 is the charge on the other one. This equation is known as Coulomb’s Law.
The electric flux, ΦE , equals the electric field multiplied by the surface area through which the field penetrates.
Flux only exists if the electric field lines penetrate straight through a surface.
If an electric field exists parallel to a surface, there is zero flux through that surface.
Gauss’s law states that the net electric flux through a closed surface is equal to the charge enclosed divided by ε0 .
ONLY use Gauss’s law when the problem has spherical, cylindrical, or planar symmetry.
First, identify the symmetry of the problem.
Then draw a closed surface, called a “Gaussian surface,” that the electric field is everywhere pointing straight through.
The electric field inside the conducting sphere must be zero everywhere.
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