108-111 - Electric Fields, Field Strength and Coulomb's Law

108-111 - Electric Fields, Field Strength and Coulomb's Law

A charged object can push or pull another charged object without touching it. The useful idea is not "mysterious action at a distance"; it is a field. A source charge changes the space around it so that another charge placed there experiences a force. This lesson turns that story into three linked calculation tools: E=F/QE = F/Q, Coulomb's law, and the field due to a point charge.

Field As A Force Region

Imagine moving a tiny positive bead near a charged metal sphere. Far away, the bead may barely feel a force. Closer in, the force becomes larger. The bead is not needed to create the field; it is a probe that reveals the field that the source charge has already set up.

Electric field

A region in which a charged particle experiences a force. Its direction at a point is the direction of the force on a positive test charge.

Two charges have different roles:

RoleMeaning
source chargethe charge that creates the electric field around it
test chargea small charge placed at a point to find what force the field would produce there

The word small matters. A test charge should not be so large that it noticeably changes the arrangement of charges creating the field. In exam calculations, this is usually assumed unless the question says otherwise.

The direction convention is simple: the electric field points in the direction of the force on a positive test charge. A negative charge in the same field feels a force in the opposite direction.

Common misconception contrast:

Tempting ideaBetter model
"There is only a field if a test charge is present."The source charge creates the field. The test charge reveals the force the field can produce.
"The field direction is the direction any charge moves."The field direction is the direction of force on a positive test charge; a negative charge is forced the other way.

For Edexcel, state what is meant by an electric field needs the force idea. A vague answer such as "an area around a charge" is not enough unless it says that a charged particle experiences a force there.

Field Strength From Force

Field strength tells you how much force the field gives to each coulomb of charge placed at a point. That is why the defining equation is:

Electric field strength

E=FQ E = \frac{F}{Q}

EE: electric field strength (N C−1\mathrm{N\,C^{-1}}), the force per unit positive charge; FF: force on the test charge (N); QQ: test charge (C). EE is a vector in the direction of the force on a positive charge.

SymbolMeaningUnit
EEelectric field strength at the pointnewton per coulomb, N C−1\mathrm{N\,C^{-1}}
FFforce on the test chargenewton, N\mathrm{N}
QQtest charge placed at that pointcoulomb, C\mathrm{C}

The unit comes straight from the definition: force per charge, so N/C\mathrm{N/C}, written N C−1\mathrm{N\,C^{-1}}.

Worked example:

A +2.0 nC+2.0\,\mathrm{nC} test charge at a point experiences a force of 6.4×10−5 N6.4 \times 10^{-5}\,\mathrm{N} to the east. Calculate the electric field strength at that point.

Decision point 1: the question gives the force on a known test charge, so use the definition:

E=FQE = \frac{F}{Q}

Decision point 2: convert nanocoulombs into coulombs:

2.0 nC=2.0×10−9 C2.0\,\mathrm{nC} = 2.0 \times 10^{-9}\,\mathrm{C}

Substitute:

E=6.4×10−52.0×10−9=3.2×104 N C−1E = \frac{6.4 \times 10^{-5}}{2.0 \times 10^{-9}} = 3.2 \times 10^4\,\mathrm{N\,C^{-1}}

Direction: the test charge is positive, so the field points in the same direction as the force. The field is 3.2×104 N C−13.2 \times 10^{4}\,\mathrm{N\,C^{-1}} east.

Now change only the test charge sign. If a −2.0 nC-2.0\,\mathrm{nC} charge at the same point experienced a force of 6.4×10−5 N6.4 \times 10^{-5}\,\mathrm{N} west, the field would still be east. The negative charge is forced opposite to the field direction.

For an Edexcel “calculate” item, the route should show the equation, the unit conversion, substitution, and a final answer with unit. If direction is asked for, treat it as physics information, not decoration.

Coulomb's Law Between Charges

When two small charged objects are separated by a distance rr, each charge exerts a force on the other along the line joining their centres. Coulomb's law gives the size of that force:

Coulomb's law

F=Q1Q24πε0r2=kQ1Q2r2 F = \frac{Q_1Q_2}{4\pi\varepsilon_0 r^2} = k\frac{Q_1Q_2}{r^2}

FF: force between the charges (N); Q1Q_1, Q2Q_2: charges (C); rr: separation of centres (m); k=1/(4πε0)=8.99×109 N m2 C−2k = 1/(4\pi\varepsilon_0) = 8.99 \times 10^{9}\,\mathrm{N\,m^{2}\,C^{-2}}. For point charges, or spherically symmetric charges viewed from outside. Small separated spheres are an approximation: nearby conductors can redistribute charge. Like charges repel; unlike charges attract.

SymbolMeaningUnit
FFforce between the two chargesN\mathrm{N}
Q1Q_1, Q2Q_2the two chargesC\mathrm{C}
rrseparation between the centres of the chargesm\mathrm{m}
ε0\varepsilon_0permittivity of free spacesupplied constant

In most A Level calculations, find the magnitude of the force using the sizes of the charges. Then use the signs to decide the direction:

  • like charges repel
  • unlike charges attract

Worked example:

Two small spheres have charges +3.0 nC+3.0\,\mathrm{nC} and −5.0 nC-5.0\,\mathrm{nC}. Their centres are 4.0 cm4.0\,\mathrm{cm} apart. Calculate the force between them and state whether it is attractive or repulsive.

Decision point 1: this asks for force between two charges, so use Coulomb's law, not E=F/QE = F/Q.

Decision point 2: convert everything into SI units:

3.0 nC=3.0×10−9 C3.0\,\mathrm{nC} = 3.0 \times 10^{-9}\,\mathrm{C} 5.0 nC=5.0×10−9 C5.0\,\mathrm{nC} = 5.0 \times 10^{-9}\,\mathrm{C} 4.0 cm=4.0×10−2 m4.0\,\mathrm{cm} = 4.0 \times 10^{-2}\,\mathrm{m}

Substitute the magnitudes:

F=(8.99×109)(3.0×10−9)(5.0×10−9)(4.0×10−2)2F = \frac{(8.99 \times 10^9)(3.0 \times 10^{-9})(5.0 \times 10^{-9})}{(4.0 \times 10^{-2})^2} F=8.4×10−5 NF = 8.4 \times 10^{-5}\,\mathrm{N}

The charges have opposite signs, so the force is attractive. Each sphere experiences the same size force, but in opposite directions along the line joining their centres.

Misconception contrast:

Tempting ideaBetter model
"The bigger charge feels the bigger force."The forces on the two charges have equal magnitude and opposite direction. The charges may accelerate differently if their masses are different.
"If rr doubles, the force halves."The force follows 1/r21/r^{2}, so doubling rr makes the force one quarter as large.

Point Charge Field

Coulomb's law gives the force between two charges. Field strength asks a slightly different question: what force would each coulomb of test charge feel at this point?

Start from a source charge QQ and a test charge qq at distance rr:

F=kQqr2F = k\frac{Qq}{r^2}

Divide by the test charge:

E=Fq=kQr2E = \frac{F}{q} = k\frac{Q}{r^2}

So the electric field strength due to a point charge is:

Field of a point charge

E=Q4πε0r2=kQr2 E = \frac{Q}{4\pi\varepsilon_0 r^2} = k\frac{Q}{r^2}

EE: field strength (N C−1\mathrm{N\,C^{-1}}); QQ: source charge (C); rr: distance from the charge (m). Radial: away from a positive charge, towards a negative one.

The important change is that the test charge has disappeared from the equation. The field at a point is set by the source charge and the distance from it. A test charge placed there feels a force because the field already exists.

Worked example:

Continue this lesson.

You’re previewing NovaLearn without an account. Create a free account to read the rest.

Create free account