Capacitor Fundamentals, Behavior, and Energy Storage

Fundamental Capacitor Equation and Current

Starting with the fundamental relationship for a capacitor, which states that charge (Q)(Q) is proportional to voltage (V)(V) and capacitance (C)(C): (Q=CV)(Q = C V). If we assume the capacitance (C) is static, meaning the plate distance (d)(d) and plate area (A)(A) are fixed, then (C=ϵAd)(C = \frac{\epsilon A}{d}) remains constant. In this scenario, the only variable changing is the voltage (V)(V).

By definition, current (I)(I) is the time rate of change of charge (Q)(Q) (I=dQdtI = \frac{dQ}{dt}). Substituting the capacitance relationship into this definition yields the fundamental equation for current in a static capacitor: (I=CdVdt)(I = C \frac{dV}{dt}). This equation highlights that current flows when the voltage across the capacitor changes.

Squishy Capacitors: A Generalized Model

The concept of a "squishy capacitor" (one where the plate distance (d)(d) is not fixed) extends the fundamental equation. Imagine a dielectric like a sponge instead of rigid Teflon. If we apply a fixed voltage (e.g., 55 volts) to this capacitor and then squish it, its capacitance becomes variable (a function of time, C(t)C(t)) because (d)(d) is changing. This concept is remarkably similar to how neurons work, functioning as 'squishy' capacitors whose membranes can be deformed by external stimuli.

To re-derive the current equation for a squishy capacitor with a fixed voltage, we start again with (Q=C(t)V)(Q = C(t) V). Since VV is fixed and CC is a function of time, when we take the derivative for current (I=dQdt)(I = \frac{dQ}{dt}), we use the product rule:

(I=ddt(C(t)V))(I = \frac{d}{dt}(C(t)V))
(I=VdC(t)dt)(I = V \frac{dC(t)}{dt})

This equation shows that current is generated even with a fixed voltage if the capacitance itself changes over time. In real-world applications, such as neurons in the ear, acoustic waveforms can squish cell membranes, changing their capacitance and generating a detectable charge, thus exciting the neuron. However, in this course, capacitors are generally considered