Electric Field Strength
- An electric field is a region of space in which an electric charge experiences a force
- The electric field strength at a point is defined as:
The force per unit charge experienced by a small positive test charge placed at that point
- The electric field strength can be calculated using the equation:
- Where:
- E = electric field strength (N C−1)
- F = electric force on the charge (N)
- q = magnitude of the charge (C)
- Note that the definition specifies that a positive test charge is used
- This sets a clear convention for the direction of an electric field, for example, in a field of strength :
- A positive charge experiences a force in the direction of the field
- A negative charge experiences a force in the opposite direction
- Hence, electric field strength is a vector quantity and is always directed:
- Away from a positive charge
- Towards a negative charge
Electric Field Strength due to a Point Charge
- The strength of an electric field due to a point charge decreases with the square of the distance
- This is an inverse square law, similar to Coulomb's law
- Using Coulomb's law, this can be written as
- Where k = Coulomb constant (N m2 C–2)
- A charged sphere acts the same as a point charge, with the same charge as the sphere, at the sphere's centre
- Within the sphere, however, the electric field strength is zero
- This means that the electric field of a charged sphere, outside the sphere, is identical to that of a point charge
Graph of field strength against distance for a positive charge
Electric field strength is zero inside a charged sphere and decreases with distance outside the sphere according to an inverse square law
Combining Electric Fields
- Both electric force and field strength are vector quantities
- Therefore, to find the electric force or field strength at a point due to multiple charges, each field can be combined by vector addition
Vector addition of electric field along the same line
For charges along the same line, the resultant field is the vector addition of the field due to both charges at a particular point
- For a point on the same line as two charges q1 and q2, with field strengths E1 and E2 respectively, the magnitude of the resultant field will be:
- The sum of the fields, E1 + E2, if they are both in the same direction
- The difference between the fields, E1 − E2, if they are in opposite directions
- The direction of the resultant field depends on
- the types of charge (positive or negative)
- the magnitude of the charges
- For a point which makes a right-angled triangle with the charges, the resultant field can be determined using Pythagoras theorem
Vector addition of electric field components
For charges which make a right-angle triangle with point X, the resultant field is the vector addition of the field due to both charges using Pythagoras theorem
Worked example
A charged particle experiences a force of 0.3 N at a point where the magnitude of electric field strength is 3.5 × 104 N C−1.
Calculate the magnitude of the charge on the particle.
Answer:
Step 1: Write down the equation for electric field strength
Step 2: Rearrange for charge Q
Step 3: Substitute in the values and calculate:
C (2 s.f.)
- The particle has a charge of 8.6 × 10−6 C or 8.6 μC
Worked example
A metal sphere of diameter 15 cm is uniformly negatively charged. The electric field strength at the surface of the sphere is 1.5 × 105 V m−1.
Determine the total surface charge of the sphere.
Answer:
Step 1: List the known quantities
- Electric field strength, E = 1.5 × 105 V m−1
- Radius of sphere, r = 15 / 2 = 7.5 cm = 7.5 × 10−2 m
- Coulomb constant, k = 8.99 × 109 N m2 C–2
Step 2: Write down the equation for electric field strength
- It is possible to treat the sphere as a point charge with the same total charge, as it is uniformly charged
Step 3: Rearrange for charge Q
Step 4: Substitute in the values and calculate:
C
- The sphere has a charge of 9.4 × 10−8 C or 94 nC
Exam Tip
When combining electric fields from multiple charges, remember that the point (e.g. point X in the examples above) represents a positive test charge, so the direction of the electric force or field will correspond to the signs of the charges; the direction of the force or field points away from a positive charge and towards a negative charge.