Capacitor Fundamentals, Behavior, and Energy Storage
Fundamental Capacitor Equation and Current
Starting with the fundamental relationship for a capacitor, which states that charge is proportional to voltage and capacitance : . If we assume the capacitance (C) is static, meaning the plate distance and plate area are fixed, then remains constant. In this scenario, the only variable changing is the voltage .
By definition, current is the time rate of change of charge (). Substituting the capacitance relationship into this definition yields the fundamental equation for current in a static capacitor: . 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 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., volts) to this capacitor and then squish it, its capacitance becomes variable (a function of time, ) because 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 . Since is fixed and is a function of time, when we take the derivative for current , we use the product rule:
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