Lesson 4 of 7
Uniform fields between plates
I can calculate a uniform parallel-plate field from potential difference and perpendicular separation.Syllabus
Syllabus 9478, 14(g). Calculate a uniform parallel-plate field from potential difference and perpendicular separation.
I can calculate the force on a charge in a uniform electric field.Syllabus
Syllabus 9478, 14(h). Calculate the force on a charge in a uniform electric field.
Between ideal broad parallel plates, potential changes uniformly across the perpendicular gap. That gap determines the field, while the charge sign determines the force direction.
In the ideal interior region, neglecting edge effects, field magnitude is:
d is the perpendicular separation between plates. The field points from higher to lower potential. Plate length along a particle's path is a different distance and does not replace d.
Worked plate field
Upper plate +120 V, lower plate 0 V
Two horizontal plates are separated by 0.0300 m. Their interior field has magnitude:
The direction is downward, from the upper plate to the lower. The chosen 0 V label is a reference; it does not by itself mean that plate is physically connected to Earth.
The field follows the perpendicular potential gradient
Use the ideal interior of broad parallel plates and neglect fringing there. The upper plate is at +120 V and the lower one at 0 V; that zero is a chosen reference, not an earth connection.
Field downward; electron force upward
E = 120/0.0300 = 4000 V/m downward. Purple arrows show the force on the named charges: +q downward and the electron upward. Their lengths are schematic; their direction is determined by qE, even when a charge is instantaneously stationary.
Upward position gives increasing potential
V(y) = 60 + 4000y, with y in metres. Therefore Ey = -dV/dy = -4000 V/m. The negative component means downward, not a negative field magnitude.
With y positive upward from the midpoint, the lower plate is at y = -0.0150 m and the upper at +0.0150 m. The midpoint potential is 60.0 V:
Ey = -dV/dy = -4000 V/m
For an electron, q = -1.60 × 10-19 C:
= (-1.60 × 10-19)(-4000)
= +6.40 × 10-16 N
Its force is upward. A positive charge would be forced downward. These statements remain true even if the particle is instantaneously stationary.
Try it step by step
Work it out in steps: Field strength E = V / d in V/m, then Acceleration of an electron a = eE / m, in units of 1015 m/s2.
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Problem 1.
Field strength E = V / d in V/m: E = 120 / 0.0050 = 24000 V/m
Acceleration of an electron a = eE / m, in units of 1015 m/s2: a = 1.60 x 10-19 x 24000 / (9.11 x 10-31) = 4.22 x 1015 m/s2
Problem 2.
Field strength E = V / d in V/m: E = 500 / 0.020 = 25000 V/m
Acceleration of an electron a = eE / m, in units of 1015 m/s2: a = 1.60 x 10-19 x 25000 / (9.11 x 10-31) = 4.39 x 1015 m/s2
Problem 3.
Field strength E = V / d in V/m: E = 90 / 0.0030 = 30000 V/m
Acceleration of an electron a = eE / m, in units of 1015 m/s2: a = 1.60 x 10-19 x 30000 / (9.11 x 10-31) = 5.27 x 1015 m/s2
Watch out for this
A student says: "Moving two charged plates further apart at a fixed p.d. makes the field between them stronger." What is wrong with this?
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For parallel plates E = V/d. At a fixed p.d., a larger separation d gives a weaker field: doubling d halves E.
Check your understanding
Horizontal plates are 0.0300 m apart and 0.0600 m long. The upper plate is at +120 V and the lower at 0 V. What are the interior field and the force direction on an electron?
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Field 4000 V/m downward; electron force upward.
The field magnitude is 120/0.0300 = 4000 V/m and points from higher to lower potential. An electron is forced in the opposite direction.
The force is set by q and E, not by the velocity direction. If this is the only significant force on a particle of constant mass, it produces constant signed acceleration. Motion parallel to E and entry perpendicular to E therefore require different component descriptions.