A Student's Guide to 
Patch-Clamp Electrophysiology
Ohm’s Law
How Membrane Properties Influence Synaptic Currents

The Introduction page discussed how neural membranes can pass current (the flow of ions through ion channels) and have resistance (largely determined by the number of open channels in the membrane). An excitatory current passing into a neuron will raise its voltage by an amount dependent on its resistance.

The relationship between voltage, current, and resistance is described by Ohm’s Law. Ohm’s Law states that Voltage (V) is equal to current (I) times resistance (R), and is traditionally written as:

V = I × R

Ohm’s law can be adapted to describe how far a neuron’s voltage will swing in response to a current flowing across its membrane:

∆Vm = ∆I × Rm

If we consider ΔVm to be an EPSP, and ΔI to be an EPSC, we can see how increasing Rm increases the voltage swing in response to an ESPC.

💡 Note: We previously discussed that resting voltage is a function largely of the Na+/K+ ATP pump and KLEAK channels. It is important to note that Ohm’s Law is not used to determine resting voltage (resting voltage can be estimated by the Goldman equation). Instead, Ohm’s Law is best used to describe voltage transients, in response to current transients (such as synaptic inputs or current injection).

Passive Membrane Properties Revisited

We previously introduced the major passive membrane properties, let’s reconsider each in the context of Ohm’s Law.

Holding Current (Ih)

Membrane Resistance (Rm)

Access Resistance (Ra)

Capacitance (Cm)