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Theme D — Fields

D.2.1 Electric Charge — IB Physics HL Revision Notes & Topical Questions

5 min read 9 parts Lesson 16 of 39 1 quiz

📚 IB Physics HL Hub / Topical Revision
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Curriculum Equation Key قوانين الرقم الهيدروجيني والاتزان الأيوني - pH & Acid-Base Equilibrium FormulasFast Exam Solution
pH = -log[H⁺] | pOH = -log[OH⁻] | pH + pOH = 14 | [H⁺][OH⁻] = 10⁻¹⁴
Word Equation & Conditions: الرقم الهيدروجيني = -لوغاريتم تركيز أيون الهيدروجين | pH + pOH = 14
Location & Specifications: الاتزان الأيوني، كيمياء 3 ثانوي، التحصيلي، و AP Chemistry.
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Lesson summary

D.2.1 Electric Charge — IB PHYSICS SL notes: Describe the properties of electric charge, including quantisation and conservation, and calculate charge from current and from numbers of electrons.Charge — the property of matter responsible for the electric force, and a scalar quant…

  • Neutral atoms
  • Charged objects
  • Sign of charge
  • Quantitative form
  • Coulomb (C)
  • Elementary charge (e)

Part 1 of 7Two kinds of charge

Two kinds of charge
Charge
  • Charge the property of matter responsible for the electric force, and a scalar quantity
Particles
  • Particles protons carry positive charge, electrons carry negative charge and neutrons carry none
Neutral atoms
  • Neutral atoms an atom has equal numbers of protons and electrons, so most everyday objects are neutral
Charged objects
  • Charged objects gaining electrons makes an object negative and losing them makes it positive
  • Protons are bound inside nuclei, so it is electrons that move between objects.
Sign of charge
  • Sign of charge a surplus of electrons is negative, and charge can be written as a count of electrons times −e

Part 2 of 7Forces between charges

Rule
  • Rule like charges repel and unlike charges attract
Strength
  • Strength the force between charged particles is much stronger than gravity between them
Quantitative form
  • Coulomb's law (D.2.4) gives its size

Part 3 of 7Unit and elementary charge

Coulomb (C)
  • Coulomb (C) the charge carried by a current of one ampere in one second
  • For a steady current Δq = IΔt.
  • Δq is in C, I in A and Δt in s.
Elementary charge (e)
  • Elementary charge (e) the magnitude of the charge of a proton or electron, e = 1.60 × 10−19 C
Quantisation
  • Quantisation any observed charge is a whole-number multiple of e
  • A body with charge q has N = q/e surplus electrons (or a deficit).
Size of a coulomb
  • Size of a coulomb about 6.25 × 1018 electrons, so ordinary electrostatic charges are in µC or nC
Quarks
  • Quarks they carry ±1/3 e and ±2/3 e but are never found alone, so free charges stay multiples of e
Current
  • Current a current of one ampere is roughly six billion billion electrons passing each second

Part 4 of 7Conservation of charge

1Conservation of charge
  • Conservation of charge the total charge of an isolated system stays constant
  • Charge can be transferred but cannot be created or destroyed.
2Rubbing
  • Rubbing when a glass rod is rubbed with silk, electrons move from the rod to the silk
  • The rod becomes positive and the silk negative by exactly the same amount.
3Identical conducting spheres
  • Identical conducting spheres when they touch, the total charge is shared equally between them
  • Each ends with the average of the original charges.
4Nuclear reactions
  • Nuclear reactions total charge before equals total charge after
  • In beta decay a neutron (charge 0) becomes a proton (+e) and an electron (−e) plus an antineutrino, so the sum stays zero.

Part 5 of 7Conductors and insulators

Conductor
  • Conductor some electrons are free to move through a metal, so charge spreads over it and can flow as current
Insulator
  • Insulator charges are held in place, so charge placed on one spot stays there
  • Plastic, glass and dry air are insulators.
Charging by friction
  • Charging by friction insulators charge easily because the transferred electrons cannot flow away
Isolated metal sphere
  • Isolated metal sphere the charge distributes uniformly over its surface because like charges repel and move as far apart as possible
Semiconductors
  • Semiconductors they lie between conductors and insulators

Part 6 of 7Charge carriers

Metals
  • Metals the moving carriers are electrons
Electrolytes and gases
  • Electrolytes and gases both positive and negative ions move
Conventional current
  • Conventional current it is defined as the flow of positive charge, whichever carriers are responsible

Part 7 of 7More from the specification

1Coulombic force quantification
  • Coulombic force quantification applying Coulomb's inverse-square electrostatic law provides a fundamental theoretical means to calculate inter-charge repulsion or attraction.
2Electrostatic and magnetic fields interactions
  • Electrostatic and magnetic fields interactions stationary charges establish radial electrostatic fields,
    • whereas moving charged particles generate circulating magnetic fields and forces.
3Coulomb electrostatic forces and field lines
  • Coulomb electrostatic forces and field lines vector field lines indicate the directional forces exerted on test charges positioned within ambient electric fields.
4Electric Field Lines Between Parallel Plates
  • A uniform electric field is established between two oppositely charged parallel metal plates;
    • electric field lines are parallel, equally spaced,
  • and directed perpendicular to the plates from positive to negative.
5Electric Field Strength and Permittivity
  • The electric field strength E between parallel conducting plates separated by distance d with potential difference V is E = V / d = σ / ε,
  • where σ is surface charge density and ε is the permittivity of the intervening material.
6Comparison with Magnetic Fields
  • Unlike electric field lines which begin on positive charges and terminate on negative charges, magnetic field lines form continuous closed loops around current paths, with flux density B dictating magnetic force magnitude.
7Uniform electric field
  • Uniform electric field electric field lines between oppositely charged parallel plates are evenly spaced and directed positive to negative.
8Electric permittivity
  • Electric permittivity permittivity describes how an insulating dielectric material between plates affects the resulting electric field strength.
9Electric field direction
  • Electric field direction defined as the direction of the electrostatic force exerted on a positive test charge.
10Potential difference
  • Work done by a unit charge passing through a component.
11Relative permittivity
  • Ratio of the permittivity of a material to that of free space.
12Permittivity
  • A property of a medium affecting the electric force within it.
13Parallel
  • Components on separate branches, each with the full e.m.f.
14Field
  • Region in which an object experiences a force at a distance
15Density
  • Mass per unit volume.
16Distance
  • Total length of path travelled, a scalar.
17Electric field
  • Region of space in which a charge experiences a force.
18Field lines
  • Lines showing the direction and strength of a magnetic field.
19Field strength
  • G = Fg/m.
20W = mg
What the symbols mean: W = weight (N) · m = mass (kg) · g = gravitational field strength (9.81 N kg−1 on Earth)

Key terms

TermMeaning
Elementary charge eThe smallest free charge, 1.60 × 10⁻¹⁹ C.
CoulombCharge delivered by a current of 1 A in 1 s.
QuantisationCharge exists only in whole multiples of e.
Conservation of chargeThe total charge of an isolated system is constant.
ConductorA material with charges free to move.
InsulatorA material in which charges stay in place.

Avoid these mistakes

1
Believing that a charged object has gained protons — it is electrons that move.
2
Thinking charge is destroyed when opposite charges meet — the total is conserved.
3
Forgetting that charge is quantised and giving fractional electrons.
4
Confusing the coulomb (charge) with the ampere (current) — 1 A = 1 C s^{−1}.
5
Saying an insulator cannot hold charge — it holds it very well, in place.

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