Electric Field and Field Intensity: MDCAT Physics notes
Electric Field and Field Intensity for MDCAT: E = F/q, units N/C and V/m, field of point charges, zero-field points, uniform fields and dielectric effect.
Electric field
An electric field is the region around a charge in which another charge experiences an electric force. The electric field intensity (field strength) at a point is the force per unit positive test charge placed there:
$$\vec{E} = \frac{\vec{F}}{q_0}$$
- It is a vector. Its direction is the direction of the force on a positive charge.
- For a positive charge $\vec{F}$ and $\vec{E}$ are parallel; for a negative charge they are opposite.
- Units: N C$^{-1}$, which equals V m$^{-1}$ and J C$^{-1}$ m$^{-1}$. The J C$^{-1}$ (volt) alone is the unit of potential, not field.
Field belongs to the source
$E$ at a point is set by the source charges, not by the test charge. Placing a different test charge changes the force $F = qE$ but not $E$.
Example: in a field of 300 N C$^{-1}$, a charge of $-2$ C feels a force of magnitude $2\times300 = 600$ N (directed opposite to $E$), while $E$ stays 300 N C$^{-1}$.
Ratio of fields at two points using the same test charge equals the ratio of forces: 50 N and 150 N give $E_A:E_B = 1:3$.
Field of a point charge
$$E = \frac{1}{4\pi\varepsilon_0}\frac{q}{r^2}$$
It points away from a positive charge and towards a negative charge. $E \propto q$, so doubling every source charge doubles the resultant field at any point.
Two charges
| Pair | Between the charges | Zero-field point |
|---|---|---|
| Equal like charges | Fields oppose | At the midpoint |
| Unequal like charges | Fields oppose | Between them, closer to the smaller charge |
| Unlike charges | Fields add (both point towards the negative) | Never between them; outside, closer to the smaller charge |
At a point near two charges, the larger and nearer charge usually dominates the direction of the net field.
Uniform field and motion of a charge
Between two oppositely charged parallel plates the field is uniform:
$$E = \frac{V}{d}$$
A charged particle in it feels a constant force $F = qE$, so its acceleration $a = qE/m$ is constant (its velocity keeps changing). To find the force you need the charge, the potential difference and the plate separation; the particle's speed is not needed.
Field inside conductors and a medium
- Inside a charged hollow conducting sphere, $E = 0$. The charge resides on the outer surface.
- In a dielectric, the field is reduced: $E_{\text{med}} = E_{\text{vac}}/\varepsilon_r$.
Key formulas
- $E = F/q_0$
- $E = kq/r^2$
- $E = V/d$ (parallel plates)
- $a = qE/m$
Common MDCAT traps
- J C$^{-1}$ is the volt, a unit of potential, not field intensity.
- For unlike charges there is no zero-field point between them.
- Changing the test charge changes the force, not the field.
- In a uniform field acceleration is constant, not velocity.
- "Force per unit positive test charge" defines field strength, not potential.
Quick revision
- $E$ is a vector; unit N C$^{-1}$ = V m$^{-1}$.
- Field between parallel plates is uniform.
- Field inside a charged hollow sphere is zero.
- Midway between equal like charges, $E = 0$.
- A dielectric reduces $E$ by $\varepsilon_r$.