When all parts of an electric circuit are at the same potential, no electric current flows and it is said to be in equilibrium. Otherwise, a current will flow from the higher potential parts to the lower ones, as when we make contact between the plates of a charged capacitor. The resulting discharging process towards equilibrium is a common phenomenon in electricity labs, as well as a topic covered in introductory physics, but some questions are not answered, e.g., could we establish a good criterion for the “end” of the charge transfer process? If so, typically how long does it take for electric equilibrium to be reached? The absence of these questions in textbooks and lab manuals has bothered me since my own undergraduate studies because, as the usual theory, in which charge is treated as a continuous, rather than discrete, parameter, predicts an exponential decay for the charge stored in the capacitor, rigorously speaking we should wait an infinitely long time for finding a complete equilibrium.1 Fortunately, when teaching experimental physics last year, I was asked about these very questions, which motivated me to search for a simple answer that could be adopted universally for measuring the “lifetime” of any physical quantity that decays exponentially in time.

1.
D.
Halliday
,
R.
Resnick
, and
J.
Walker
,
Fundamentals of Physics
, 9th ed. (
Wiley
,
New York
,
2011
), Sec. 27–9.
2.
The role of the resistor in this circuit is to limit the discharge current, avoiding a rapid heating (by Joule effect) of the circuit wires, which can explode them.
3.
J. G.
King
and
A. P.
French
, “
Using a multimeter to study an RC circuit
,”
Phys. Teach.
33
,
188
189
(
March 1995
).
4.
As usual, the instrumental error for analogical meters is taken here as half the smallest division on the scale. E.g., if the smallest division is 0.1 V, then (Δ V)exp = 0.05 V. For digital meters, we take the smallest value it can read on a given setting.
5.
Y.
Kraftmakher
, “
Charge and energy stored in a capacitor
,”
Phys. Teach.
50
,
73
74
(
Feb. 2012
).
6.
Alternatively, one might choose to define the full discharge time to be when the charge left on a plate (in the exponential model) is less than the charge of a single electron. However, in the example considered here, it would mean waiting over 33 time constants, or more than 15 minutes, so we prefer our definition.
7.
For those using an ammeter, the corresponding ratio is I/(Δi)exp, where I = E/R is the maximum (absolute) value of the electric current. This is because i(t)=dq/dt=Q/(RC)et/(RC)=ε/Ret/τ0=Iet/τ0, so τ = τ0 ln[I/(Δi)exp].
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