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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

📚 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.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

FeatureElectric fieldMagnetic field
ForceqE, along or against EqvB, perpendicular to v and B
Acts on stationary charge?YesNo
Work doneYes, speed changesNone, speed constant
Path (entry perpendicular to field)ParabolaCircle
  • 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

TermMeaning
Electric field strength EForce per unit positive charge, in N C⁻¹ or V m⁻¹.
Electronvolt1.6 × 10⁻¹⁹ J, the energy gained by an electron through 1 V.
Uniform fieldField of constant size and direction, as between parallel plates.
Parabolic trajectoryPath of a charge entering perpendicular to a uniform field.
Electron gunDevice 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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