can be used to explain how a charged particle can
exert an electric force 𝐹
on a second charged particle even though there is no contact between
the particles.
LO 22.1.3 Explain how a small positive test charge is used (in principle) to measure the electric
field at any given point.
LO 22.1.4 Explain electric field lines, including where they originate and terminate and what
their spacing represents.
LO 22.2.0 Solve problems related to the electric field due to a charged particle.
LO 22.2.1 In a sketch, draw a charged particle, indicate its sign, pick a nearby point, and then
draw the electric field vector 𝐸
when the particle is positively charged and when it is negatively charged.
LO 22.2.3 For a given point in the electric field of a charged particle, apply the relationship
between the field magnitude E, the charge magnitude q, and the distance r between the point and
the particle.
LO 22.2.4 Identify that the equation given here for the magnitude of an electric field applies only
to a particle, not an extended object.
LO 22.2.5 If more than one electric field is set up at a point, draw each electric field vector and
then find the net electric field by adding the individual electric fields as vectors (not as scalars).
LO 22.3.0 Solve problems related to the electric field due to an electric dipole.
LO 22.3.1 Draw an electric dipole, identifying the charges (sizes and signs), dipole axis, and
direction of the electric dipole moment.
LO 22.3.2 Identify the direction of the electric field at any given point along the dipole axis.
LO 22.3.3 Outline how the equation for the electric field due to an electric dipole is derived from
the equations for the electric field due to the individual charged particles.
LO 22.3.4 For a single charged particle and an electric dipole, compare the rate at which the
electric field magnitude decreases with increase in distance.
LO 22.3.5 Apply the relationship between the magnitude p of dipole moment, the charge
separation d, and the magnitude q of either of the charges.
LO 22.3.6 For any distant point along a dipole axis, apply the relationship between the electric
field magnitude E, the distance z from the center of the dipole, and either the dipole moment
magnitude p or the product of charge magnitude q and charge separation d.
LO 22.4.0 Solve problems related to the electric field due to a line of charge.
LO 22.4.1 For a uniform distribution of charge, find the linear charge density λ for charge along
a line, the surface charge density σ for charge on a surface, and the volume charge density ρ for
charge in a volume.
LO 22.4.2 For charge that is distributed uniformly along a line, find the net electric field at a
given point near the line by splitting the distribution up into charge elements dq and then
summing (by integration) the electric field vectors 𝐸