Theme D — Fields
D.3.5 Charged Particles in Electric Fields — IB Physics HL Revision Notes & Topical Questions
5 min read 10 parts Lesson 32 of 39 1 quiz
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.
Lesson summary
D.3.5 Charged Particles in Electric Fields — IB PHYSICS SL notes: Describe and calculate the motion of charges accelerated and deflected in uniform electric fields.Force — an electric field exerts F = qE on a charge whether it moves or notE is in N C−1, which equals V m−1.Directi…
- Acceleration
- Speed change
- Between parallel plates
- Uncharged particles
- Energy gain
- Only V counts
Part 1 of 8Force and acceleration
Force and acceleration
Force
- Force an electric field exerts F = qE on a charge whether it moves or not
- E is in N C−1, which equals V m−1.
Direction
- Direction the force is along the field for a positive charge and opposite to it for a negative charge
Acceleration
- Acceleration a = qE/m from Newton's second law
Speed change
- Speed change unlike the magnetic force, the electric force can change speed because it can have a component along the motion and so does work
Between parallel plates
- Between parallel plates the field is uniform with E = V/d, directed from the positive to the negative plate
Uncharged particles
- Uncharged particles a neutron feels no force and passes straight through undeflected
Part 2 of 8Acceleration along the field
Energy gain
- Energy gain a charge released from rest through a p.d.
- V gains kinetic energy qV
Speed
- Speed qV = ½mv2, so v = √(2qV/m)
Only V counts
- Only V counts the result is independent of how the field is arranged
Electronvolt
- 1 eV = 1.6 × 10−19 J, the energy gained by an electron through 1 V
- An electron accelerated through 2000 V has kinetic energy 2000 eV.
Applications
- Applications electron guns in old televisions and X-ray tubes
Part 3 of 8Deflection at right angles to the field
Model
- Model the motion is like a projectile under gravity, with qE replacing mg
- Along the field the particle accelerates at a = qE/m.
- Perpendicular to the field it moves at constant speed vx.
Time in the field
- Time in the field for plates of length ℓ, t = ℓ/vx
Sideways velocity
- Sideways velocity vy = at = qEℓ/(mvx)
Sideways displacement
- Sideways displacement y = ½at2 = qEℓ2/(2mvx2)
Path
- Path a parabola inside the field and a straight tangent line after it leaves
- The straight line appears to come from the midpoint of the plates.
Deflection angle
- Deflection angle tan θ = vy/vx
Part 4 of 8Direction and amount of deflection
Direction and amount of deflection
Positive charge
- Positive charge it is deflected towards the negative plate
Negative charge
- Negative charge it is deflected towards the positive plate
Force
- Force it is the same at all points and always in the same direction
Greater mass
- Greater mass the deflection is smaller
Greater charge
- Greater charge the deflection is greater
Greater speed
- Greater speed the deflection is smaller, since the particle spends less time in the field
Comparing particles
- Comparing particles a particle with a much larger mass than charge ratio is much less deflected and hits the plate later, with a smaller curve
- A boron nucleus has 5 times the charge but 11 times the mass of a proton, so it deflects less.
Part 5 of 8Comparing electric and magnetic deflection
| Feature | Electric field | Magnetic field |
|---|---|---|
| Force | qE, along or against E | qvB, perpendicular to v and B |
| Acts on stationary charge? | Yes | No |
| Work done | Yes, speed changes | None, speed constant |
| Path (entry perpendicular to field) | Parabola | Circle |
- Gravity
- it is normally negligible for charged particles, because even in a weak field the electric force on an electron is enormously larger than its weight
Part 6 of 8Applications
1Accelerators
- Accelerators electric fields give energy to charges
2Oscilloscopes
- Oscilloscopes deflection plates steer an electron beam to draw a trace
3Inkjet printers
- Inkjet printers charged droplets are deflected onto paper
4Electrostatic precipitators
- Electrostatic precipitators charged dust is pulled onto collecting plates
Part 7 of 8Energy method
Work by the field
- Work by the field qEd = qΔV, equal to the change in kinetic energy
Plates
- Plates when a charge is released between plates, find the final speed from energy
- Use E = V/d only if the force or time is also needed.
Massive droplets
- Massive droplets gravity must be included when the particle is a massive charged droplet
Part 8 of 8More from the specification
More from the specification
Fleming's Left-Hand Rule
- For a current-carrying conductor or positive charge moving across a magnetic field, Fleming's left-hand rule determines force direction: First finger = field (B), seCond finger = conventional current (I),
- and thuMb = resultant magnetic force.
Magnetic Force on a Current-Carrying Conductor
- The magnetic force experienced by a straight conductor carrying current I through a uniform magnetic field B is given by F = B I L sin(θ),
- where θ is the angle between current and field.
Magnetic Force on Moving Charged Particles
- A particle carrying charge q moving with velocity v through a magnetic field B experiences a magnetic deflecting force F = q v B sin(θ), directed perpendicularly to both velocity and field.
Forces Between Parallel Conductors
- Two parallel conductors carrying electric currents in the same direction exert attractive magnetic forces upon each other,
- whereas currents in opposite directions repel.
Fleming's Left-Hand Rule
- For a current-carrying conductor or positive charge moving across a magnetic field, Fleming's left-hand rule determines force direction: First finger = field (B), seCond finger = conventional current (I),
- and thuMb = resultant magnetic force.
Magnetic Force on a Current-Carrying Conductor
- The magnetic force experienced by a straight conductor carrying current I through a uniform magnetic field B is given by F = B I L sin(θ),
- where θ is the angle between current and field.
Magnetic Force on Moving Charged Particles
- A particle carrying charge q moving with velocity v through a magnetic field B experiences a magnetic deflecting force F = q v B sin(θ), directed perpendicularly to both velocity and field.
Forces Between Parallel Conductors
- Two parallel conductors carrying electric currents in the same direction exert attractive magnetic forces upon each other,
- whereas currents in opposite directions repel.
Fleming's Left-Hand Rule
- For a current-carrying conductor or positive charge moving across a magnetic field, Fleming's left-hand rule determines force direction: First finger = field (B), seCond finger = conventional current (I),
- and thuMb = resultant magnetic force.
Magnetic Force on a Current-Carrying Conductor
- The magnetic force experienced by a straight conductor carrying current I through a uniform magnetic field B is given by F = B I L sin(θ),
- where θ is the angle between current and field.
Magnetic Force on Moving Charged Particles
- A particle carrying charge q moving with velocity v through a magnetic field B experiences a magnetic deflecting force F = q v B sin(θ), directed perpendicularly to both velocity and field.
Forces Between Parallel Conductors
- Two parallel conductors carrying electric currents in the same direction exert attractive magnetic forces upon each other,
- whereas currents in opposite directions repel.
F = Bqv
What the symbols mean: F = force on the moving charge (N) · B = magnetic flux density (T) · q = charge (C) · v = speed (m s−1)
Current
- Flow of electrons in a circuit.
Conductor
- Material that allows current to flow.
Density
- Mass per unit volume.
Charge-to-mass ratio
- Q/m, which determines the acceleration in a given field
Field lines
- Lines showing the direction and strength of a magnetic field.
Field strength
- G = Fg/m.
F = BIL
What the symbols mean: F = force on the wire (N) · B = magnetic flux density (T) · I = current (A) · L = length of wire in the field (m) · θ = angle between wire and field
Key terms
| Term | Meaning |
|---|---|
| Electric field strength E | Force per unit positive charge, in N C⁻¹ or V m⁻¹. |
| Electronvolt | 1.6 × 10⁻¹⁹ J, the energy gained by an electron through 1 V. |
| Uniform field | Field of constant size and direction, as between parallel plates. |
| Parabolic trajectory | Path of a charge entering perpendicular to a uniform field. |
| Electron gun | Device that accelerates electrons through a p.d. into a beam. |
Avoid these mistakes
1
Giving the force on a negative charge in the direction of E — the force is opposite to E.
2
Using E = V/d for a non-uniform field — it applies only between parallel plates.
3
Treating electric deflection as circular motion — it is parabolic.
4
Forgetting to convert cm to m or eV to joules.
5
Including gravity when it is negligible, or ignoring it for a massive charged droplet.
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