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Flashcards · 9702 · A Level Topic 18

Electric fields (A Level) flashcards

23 cards on A Level Topic 18, subtopics 18.1 to 18.5. Pick a subtopic or study them all.

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18.1 Electric fields and field lines

Electric field
A region of space in which a charge experiences a force due to other charges. A field of force.
Which way do electric field lines point?
In the direction of the force on a small positive test charge: away from positive charges, towards negative charges. Closer lines mean a stronger field.
Field-line pattern around an isolated point charge
Radial lines: outward from a positive charge, inward to a negative charge, spreading apart with distance.
Field-line pattern between two charged parallel plates
Parallel, equally spaced lines from the positive to the negative plate: a uniform field (with some curving at the edges).

18.2 Uniform electric fields

Field strength between charged parallel plates
E = V ÷ d, where V is the p.d. between the plates and d their separation. Unit V m⁻¹ (= N C⁻¹). It holds only for a uniform field.
Plates 5.0 mm apart have a p.d. of 200 V. Find the field strength.
E = V ÷ d = 200 ÷ 0.0050 = 4.0 × 10⁴ V m⁻¹.
A charged particle enters a uniform electric field at right angles to it. Describe its path.
A parabola, like a projectile: constant velocity across the field, constant acceleration a = qE ÷ m along it.
An electron is accelerated from rest through 500 V. Find its speed.
eV = ½mv², so v = √(2eV ÷ m) = √(2 × 1.60 × 10⁻¹⁹ × 500 ÷ 9.11 × 10⁻³¹) = 1.33 × 10⁷ m s⁻¹.
The electronvolt
The energy gained by an electron accelerated through a p.d. of 1 V: 1 eV = 1.60 × 10⁻¹⁹ J.

18.3 Electric force between point charges

Coulomb’s law
F = Qq ÷ (4πε₀r²): the force between two point charges is proportional to the product of the charges and inversely proportional to the square of their separation.
Value of 1/(4πε₀), and the unit of ε₀
1/(4πε₀) ≈ 8.99 × 10⁹ N m² C⁻². ε₀ = 8.85 × 10⁻¹² F m⁻¹.
Two +2.0 μC point charges are 0.10 m apart. Find the force between them.
F = 8.99 × 10⁹ × (2.0 × 10⁻⁶)² ÷ 0.10² = 3.6 N, repulsive.
Electric vs gravitational force between point objects
Both are inverse square laws. Gravity is always attractive; the electric force is attractive or repulsive, depending on the signs of the charges.

18.4 Electric field of a point charge

Electric field strength
The force per unit positive charge on a small test charge at that point: E = F ÷ q. Unit N C⁻¹. A vector.
Field strength of a point charge Q
E = Q ÷ (4πε₀r²), with r measured from the charge.
Find the field strength 0.20 m from a point charge of +5.0 × 10⁻⁶ C.
E = 8.99 × 10⁹ × 5.0 × 10⁻⁶ ÷ 0.20² = 1.12 × 10⁶ N C⁻¹, directed radially outward.
How is an isolated charged sphere treated for points outside it?
As a point charge at its centre, so r is measured from the centre, not the surface.
Force on a charge q in a field of strength E
F = Eq, in the direction of E for a positive charge and opposite to E for a negative charge.

18.5 Electric potential

Electric potential
The work done per unit positive charge in bringing a small test charge from infinity to that point. V = Q ÷ (4πε₀r). Unit V (J C⁻¹). A scalar.
How does the sign of electric potential differ from gravitational potential?
Gravitational potential is always negative (gravity only attracts). Electric potential is positive near a positive charge and negative near a negative charge.
Electric potential energy of a pair of point charges
Ep = Qq ÷ (4πε₀r), the work done bringing one charge from infinity to distance r from the other.
Relationship between field strength and potential
E = −dV/dr: the field strength is minus the potential gradient. The field points towards decreasing potential.
Equipotentials
Lines or surfaces of constant potential. They are perpendicular to field lines, and no work is done moving a charge along one.