Radioactive Decay and Capacitor Discharge

Radioactive Decay

The solution of is:

is proportional to , therefore:

The half-life of a radioactive sample can be defined as:

The time taken for the number of radioactive particles present, , to halve from an original value.
The time taken for the activity, , of a source to halve from an original value.

at time . After one half-life, at .
therefore becomes .
Solving for , we obtain:

Capacitors

A capacitor is a passive electronic device which stores energy. They consist of two or more conducting plates separated by an insulating material (the dielectric). Placing an insulator between the plates increases the charge stored on the plates. When connected to a battery:

The plate connected to the positive side of the battery loses electrons to the battery.
The other plate gains electrons from the negative side of the battery.

For a charging capacitor:

The current decreases exponentially with time.
The rate of flow of electrons is greatest at the start, and decreases to zero when the capacitor is fully charged.
The potential difference of the capacitor and battery are equal.

When a capacitor is charged, the capacitor remains neutral. There is no net charge stored. However, the charge difference has created an electric field that is capable of moving (doing work on) any other charged particle that is placed between the capacitor plates. The capacitor stores electric potential energy.

The capacitance (C) of an object, measured in farads (F), is the amount of charge it is able to store per unit potential difference across it:

Where C is capacitance (F), Q is charge (C), and V is potential difference (V).

The energy stored in a capacitor is given by:

Dielectric breakdown

The capacitance of a set of charged parallel plates increases by the insertion of a dielectric material. The capacitance is inversely proportional to the electric field between the plates, and the presence of the dielectric reduces the electric field.

Where:

is the relative permittivity of the dielectric
is the permittivity of free space
is the cross-sectional area
is the distance between the plates

As the p.d increases, the stored energy increases. When the charge is large enough, the dielectric will break down and the charge will start to flow between the plates.

Capacitor Discharge

When a charged capacitor is allowed to discharge through a resistor:

Current decreases with time, approaching zero when the capacitor is fully discharged.
A graph of current against time shows exponential decay. Current reduces by the same factor in equal time intervals.
If a quantity decreases at a rate a which is proportional to the quantity remaining then the decay is exponential.

The charge in one small time period decreases from to , and is proportional to the charge remaining:

For a discharging capacitor with circuit resistance , capacitance , and initial charge, p.d., and current , , and .

The product is the time constant, and gives an indication of how long the capacitor takes to discharge. .

The time constant is the time for the initial charge / voltage / current to fall to of the initial value when discharging.

The half-life (the time taken for the current / voltage /current to fall to half its initial value) is given by:

Capacitor Charging

For a charging capacitor with circuit resistance , capacitance , and final charge, p.d., and initial current , , and .

For charge and p.d., the time constant now represents the time to charge to of the final value, or 63%. The equation for current is the same for a charging or discharging capacitor.