Rather than thinking of one charge exerting a direct "action at a distance" force on another, it is far more powerful to introduce the electric field: a property of space itself. A source charge creates a field everywhere around it; a second charge then responds to the field at its location. This field concept becomes indispensable when we get to time-varying fields and electromagnetic waves.
Key Concepts
Electric Field Definition
The electric field E at a point is defined as the force per unit positive test charge placed at that point: E=F/q0โ. Units: N/C (equivalently V/m). The test charge q0โ must be small enough not to disturb the source charges.
Field of a Point Charge
A point charge q creates a field E=kโฃqโฃ/r2 at distance r. The field points radially outward from a positive charge and inward toward a negative charge.
Electric Field Lines
Field lines are a visual representation: they point in the direction of E, originate on positive charges and terminate on negative charges, never cross, and are denser where the field is stronger.
Superposition of Fields
The total electric field at a point due to several charges is the vector sum of the individual fields: Enetโ=E1โ+E2โ+โฏ. For continuous distributions, this sum becomes an integral.
Electric Dipole
Two equal and opposite charges +q and โq separated by distance d. The dipole moment is pโ=qd (pointing from โq to +q), with magnitude p=qd. Dipoles in a uniform external field experience a torque ฯ=pEsinฮธ that tends to align them with the field.
Key Equations
Electric field from force
E=q0โFโ
Definition of the electric field at a point in terms of force on a positive test charge qโ.
Field of a point charge
E=kr2โฃqโฃโ
Magnitude of the field at distance r from point charge q. Direction: away from positive q, toward negative q.
Electric dipole moment
p=qd
Magnitude of the dipole moment. p points from โq to +q. Torque in field: ฯ = pE sin ฮธ.
Torque on dipole in uniform field
ฯ=pEsinฮธ
Torque on a dipole of moment p in field E; ฮธ is the angle between p and E. Tends to align the dipole with the field.
Worked Example
Net Electric Field Between Two Opposite Charges
Problem
Charge q1โ=+5 nC is at the origin and q2โ=โ5 nC is at x=0.20 m. Find the electric field at the midpoint x=0.10 m.
Solution
Field from q1โ (positive, at origin) points away from it โ in the +x direction at x=0.10 m:
Both fields point in the same direction (+x), so they add:
Enetโ=E1โ+E2โ=4495+4495=8990ย N/C
AnswerE_net = 8990 N/C in the +x direction.
Practice
Exercises
7 problems
1of 7
A point charge q=+8 nC. What is the magnitude of the electric field (in N/C) at a distance r=0.40 m from it?
N/C
2of 7
A charge q0โ=+3ฮผC is placed in a uniform electric field E=2.0ร105 N/C. What is the magnitude of the force (in N) on it?
N
3of 7
Charges q1โ=+5 nC (at x=0) and q2โ=โ5 nC (at x=0.20 m) form a dipole. What is the magnitude of the electric field (in N/C) at the midpoint x=0.10 m?
N/C
4of 7
Charges q1โ=+4 nC (at x=0) and q2โ=+1 nC (at x=0.60 m) are fixed. At what position x (in m) between them is the electric field zero?
m
5of 7
A dipole consists of q=+5 nC and โ5 nC separated by d=0.040 m. What is the dipole moment (in nCยทm)?
nCยทm
6of 7
A charge q=โ4ฮผC is placed in a uniform field E=600 N/C. What is the magnitude of the force (in mN) on the charge?
mN
7of 7
The electric field at a distance of r=0.15 m from a point charge is measured to be E=800 N/C. What is the magnitude of the charge (in nC)?
nC
Key Takeaways
The electric field is a property of space โ it exists at every point whether or not a test charge is placed there.
At any point, F=qE: positive charges are pushed along E; negative charges are pushed opposite to E.
For opposite-sign charge pairs (dipoles), the fields at the midpoint add; for same-sign pairs, they partially cancel.
Field lines can never cross โ if they did, a test charge at that point would have to accelerate in two directions simultaneously.
To find a null-field point between two like charges, set the two field magnitudes equal and solve for position.