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GRADE 8 · CHARGE AND ELECTRIC FIELD

Atomic structure and charge conservation

Electrons, ions, charge quantization and charge conservation.

22 minutes4 theory cards
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Understanding step by step

How can an object be neutral if it consists of charged particles? Count positive and negative charges separately and see what losing one electron changes.

The whole atom is neutral3 protons3 electronstotal charge 0What if one electron is removed?
A schematic neutral atom has three protons and three electrons whose charges cancel. The three plus signs represent nuclear protons; neutrons are omitted because they do not affect charge. The blue area represents the electron shell, with sizes enlarged for clarity.

Nucleus and electron shell

An atom has a positively charged nucleus surrounded by negative electrons. Protons carry the nucleus's positive charge; neutrons are electrically neutral. One proton and one electron have charges of equal magnitude, so equal numbers of protons and electrons give a total of zero. This is a neutral atom. Neutrality means cancellation, not absence of charge. A nucleus-and-shell drawing shows composition, not the atom's actual scale.

+0+0+0Nucleus3 protons3 neutrons3 electronsTotal charge 0; sizes schematic
The nucleus contains three protons marked plus and three neutrons marked zero. The electron shell contains three negative electrons. The charges of the three protons and three electrons cancel; neutrons do not affect the sum. The blue area represents the shell schematically; particle positions and scales are not literal.

How a positive ion forms

Suppose a neutral atom loses an electron. Its nucleus is unchanged, but it now has less negative than positive charge. The remainder is positively charged and is called a positive ion. Gaining an extra electron instead produces a negative ion. Check the sign by reasoning: removing a negative increases the sum; adding a negative decreases it. Ordinary charging changes electrons, not the composition of the atomic nucleus.

Lost an electronGained an electronpositivenegative2 electrons4 electronsEach nucleus has 3 protons
Both nuclei contain the same three protons. On the left, after an electron is lost, two remain in the shell and one is shown leaving: the ion is positive. On the right, the gained electron is already included among four shell electrons: the ion is negative. Blue areas and particle positions are schematic; nuclear composition is unchanged.

The smallest ordinary charge unit

Can charge be transferred in arbitrarily small amounts? Ordinary experiments transfer whole numbers of electrons or ions. The magnitude of electron and proton charge is the elementary charge e ≈ 1,6·10⁻¹⁹ Кл. An electron carries −e and a proton +e. This value is tiny, so a macroscopic object's charge comprises an enormous number of units. The symbol e denotes a positive magnitude; the particle's sign is written separately.

One electron transferred during contacte⁻+−lost an electrongained an electronThe pair's total charge remains zero
Both objects were initially neutral and exchanged no charge with their surroundings. During contact, one electron moved from left to right. After separation, the left object has positive net charge and the right has an equal-magnitude negative charge. The signs inside indicate the objects' final charges; e⁻ denotes an electron, whose own charge is negative.

Why charge comes in multiples of e

If n electrons pass between objects, the magnitude of transferred charge is ne. Twice as many electrons transfer twice as much charge; at n = 0 there is no transfer. But n must be an integer: this process does not produce half an electron. Dividing a large object's charge between two objects divides a collection of carriers. It cannot give an arbitrary fraction of an individual electron's charge.

Electron charge: q = −neq = −eq = −2eq = −3eCharge magnitude: |q| = nen: an integer number of electrons
One, two and three electrons carry −e, −2e and −3e respectively; their charge magnitudes are e, 2e and 3e. Here e is the positive elementary charge magnitude. Ordinary charging transfers whole electrons, not arbitrary parts of them.

The algebraic sum is conserved

Track two objects as one system. An electron leaves the first and arrives at the second: their total-charge changes are opposite. Thus, in a system exchanging no charge with its surroundings, the algebraic sum of charges is conserved. Algebraic means including signs: +q and −q sum to zero although each is nonzero. Contact may change the distribution but cannot create net charge from nothing.

An example of redistribution+3e−eafter exchange+e+eΣq = +2eΣq = +2eThe shares depend on conditions
Example of redistribution in an isolated pair: before exchange, +3e and −e give +2e; afterwards, +e and +e also give +2e. This is one possible outcome of two electrons moving from the second object to the first. The law conserves the algebraic sum; individual shares depend on conditions and are not always equal.

The system boundary matters

A charged metal object touches Earth and nearly discharges. Has the law failed? No: we counted only the object, while carriers could move into Earth or arrive from it. One object's charge need not stay constant when it exchanges charge. Include everyone involved in the exchange and conservation is restored. Before adding charges, identify the boundary through which carriers may have passed.

IsolatedConnected to Earthe⁻q conservedobject's q changesInclude all participants in charge exchange
On the left, a negatively charged object exchanges no charge with its surroundings. On the right, grounding has begun: electrons can leave through the conducting connection, so the object's charge changes. Charge conservation must include both object and Earth. In general, transfer direction depends on initial conditions.

Charged objects in contact

Isolated objects have charges +5 nC and −2 nC. What is their total charge after contact?

Before contactIsolated system boundaryObject 1+5 нКлObject 2−2 нКлTotal charge after contact — ?
Before contact, two isolated objects have charges +5 nC and −2 nC. The dashed boundary encloses both: no charge crosses into the surroundings. Their outlines are schematic; physical shapes and sizes are unspecified. Find total charge after contact.

Worked example · 1

Add the initial charges algebraically: +5 + (−2) = +3 нКл. Negative charge cancels part of the positive charge.

Sum before contactIsolated system boundaryObject 1+5 нКлObject 2−2 нКл+5 + (−2) = +3 нКлAdd with signs
Both objects, their initial charges +5 nC and −2 nC, and the system boundary are unchanged. The algebraic sum before contact is +5 + (−2) = +3 нКл. Add charges with their signs.

Worked example · 2

The objects are isolated from their surroundings, so contact can only redistribute this +3 nC, not change the total.

After contactIsolated system boundaryObject 1q₁Object 2q₂q₁ + q₂ = +3 нКлNo exchange with surroundings
The same objects inside the same boundary are brought into contact. Their drawn sizes remain unchanged; only their separation changes. Isolation excludes charge exchange with the surroundings, so the total after contact remains +3 nC. q₁ and q₂ represent the as-yet unknown individual charges.

Worked example · 3

The total alone cannot determine each object's final charge: their shapes, sizes and positions are also needed.

Not enough data for each shareIsolated system boundaryObject 1q₁Object 2q₂q₁ + q₂ = +3 нКлq₁ and q₂ are unspecified
The touching objects and isolated-system boundary are unchanged. The known sum is q₁ + q₂ = +3 нКл. The conditions determine neither individual shares nor their equality. Identical schematic outlines do not specify the objects' physical shapes or sizes.

Check the result

Total charge: +3 nC. The isolated pair retains the same net positive charge after contact.

Key idea · 1

Neutral matter contains charges that cancel in the sum.

Key idea · 2

Losing an electron makes a neutral atom a positive ion; gaining one makes it a negative ion.

Key idea · 3

The signed sum is conserved in a system with no charge transfer across its boundary.

What comes next

Next, use charge to calculate interaction forces and introduce a quantity describing the electric field.

Basic Concepts

3 concepts

Electrical structure of the atom

An atom consists of a positively charged nucleus and negative electrons. In a neutral atom, total positive and negative charges are equal in magnitude.

Losing electrons forms a positive ion, gaining extra electrons forms a negative ion.

Law of conservation of charge

The algebraic sum of the electric charges of a closed system remains constant.

Charging does not create charge from nothing: electrons pass between objects, conserving total charge.

Elementary charge

An object's electric charge changes in amounts whose magnitudes are multiples of one electron's charge magnitude.

Divisibility of charge does not mean the possibility of obtaining an arbitrary small fraction in ordinary school experiments.

Physical quantities

1 magnitude

Elementary charge

e

The magnitude of the electric charge of an electron or proton.

Unit: coulomb · \mathrm{Кл}

Problems on this topic

Statements, answer options and the walkthrough.