Jove
Visualize
Contact Us
JoVE
x logofacebook logolinkedin logoyoutube logo
ABOUT JoVE
OverviewLeadershipBlogJoVE Help Center
AUTHORS
Publishing ProcessEditorial BoardScope & PoliciesPeer ReviewFAQSubmit
LIBRARIANS
TestimonialsSubscriptionsAccessResourcesLibrary Advisory BoardFAQ
RESEARCH
JoVE JournalMethods CollectionsJoVE Encyclopedia of ExperimentsArchive
EDUCATION
JoVE CoreJoVE BusinessJoVE Science EducationJoVE Lab ManualFaculty Resource CenterFaculty Site
Terms & Conditions of Use
Privacy Policy
Policies

Related Concept Videos

Action Potential01:14

Action Potential

Neurons communicate by firing action potentials—the electrochemical signal that is propagated along the axon. The signal results in the release of neurotransmitters at axon terminals, thereby transmitting information to the nervous system. An action potential is a specific "all-or-none" change in membrane potential that results in a rapid spike in voltage.
Membrane potential in neurons
Neurons typically have a resting membrane potential of about -70 millivolts (mV). When they receive...
Action Potential01:14

Action Potential

Neurons communicate by firing action potentials—the electrochemical signal that is propagated along the axon. The signal results in the release of neurotransmitters at axon terminals, thereby transmitting information to the nervous system. An action potential is a specific "all-or-none" change in membrane potential that results in a rapid spike in voltage.
Membrane potential in neurons
Neurons typically have a resting membrane potential of about -70 millivolts (mV). When they receive...
Action Potentials01:41

Action Potentials

Overview
Energy Stored In A Coaxial Cable01:31

Energy Stored In A Coaxial Cable

A coaxial cable consists of a central copper conductor used for transmitting signals, followed by an insulator shield, a metallic braided mesh that prevents signal interference, and a plastic layer that encases the entire assembly.
In the simplest form, a coaxial cable can be represented by two long hollow concentric cylinders in which the current flows in opposite directions. The magnetic field inside and outside the coaxial cable is determined by using Ampère's law. The magnetic field inside...
Design Example: Frog Muscle Response01:14

Design Example: Frog Muscle Response

A student is tasked to work on an intriguing experiment involving an RL (Resistor-Inductor) circuit to study the muscle response of a frog's leg to electrical stimulation. The RL circuit plays a crucial role in this experiment, providing the means to control and measure the electrical impulses that trigger muscle contraction.
When the switch connecting the RL circuit is closed, a brief muscle contraction is observed. This is because, at a steady state, the inductor acts like a short circuit,...
Inductance: Solid Cylindrical Conductor01:24

Inductance: Solid Cylindrical Conductor

To calculate the inductance of a solid cylindrical conductor, consider a 1-meter section of a non-magnetic, current-carrying conductor with radius r. Disregarding end effects and assuming uniform current density, Ampere's law helps determine the magnetic field inside the conductor. This law states that the magnetic field intensity H is concentric and constant within the conductor.
Given the uniform current distribution, the magnetic field Hx and flux density Bx inside the conductor are...

You might also read

Related Articles

Articles linked to this work by shared authors, journal, and citation graph.

Sort by
Same author

Reproductive morphology and its application in testing molecular systematic hypotheses in the family Gobiidae (Teleostei, Gobiiformes).

Journal of fish biology·2017
Same author

Rediscovering hermaphroditism in Grammatidae with the description of the testicular gland in Brazilian Basslet Gramma brasiliensis.

Brazilian journal of biology = Revista brasleira de biologia·2016
Same author

Development of early social behaviour of rainbow trout, Salmo Gairdneri (Pisces, Salmonidae).

Behavioural processes·2014
Same author

Attraction of female fathead minnows,Pimephales promelas, to chemical stimuli from breeding males.

Journal of chemical ecology·2013
Same author

Demonstration, with the electron microscope, of a nucleus in Bacillus mycoides grown in a nitrogen-free medium.

Journal of bacteriology·2010
Same author

A study, with the high-voltage electron microscope, of the endospore and life cycle of Bacillus mycoides.

Journal of bacteriology·2010

Related Experiment Video

Updated: Jun 19, 2026

Modeling Biological Membranes with Circuit Boards and Measuring Electrical Signals in Axons: Student Laboratory Exercises
13:56

Modeling Biological Membranes with Circuit Boards and Measuring Electrical Signals in Axons: Student Laboratory Exercises

Published on: January 18, 2011

LONGITUDINAL IMPEDANCE OF THE SQUID GIANT AXON.

K S Cole1, R F Baker

  • 1Department of Physiology, College of Physicians and Surgeons, Columbia University, New York, and the Marine Biological Laboratory, Woods Hole, Massachusetts.

The Journal of General Physiology
|October 30, 2009
PubMed
Summary

This study reveals inductive properties within squid giant axon membranes using alternating current impedance measurements. These findings suggest a novel equivalent circuit model for neuronal membranes.

More Related Videos

In Situ Visualization of Axon Growth and Growth Cone Dynamics in Acute Ex Vivo Embryonic Brain Slice Cultures
10:45

In Situ Visualization of Axon Growth and Growth Cone Dynamics in Acute Ex Vivo Embryonic Brain Slice Cultures

Published on: October 14, 2021

Acute Dissociation of Lamprey Reticulospinal Axons to Enable Recording from the Release Face Membrane of Individual Functional Presynaptic Terminals
12:01

Acute Dissociation of Lamprey Reticulospinal Axons to Enable Recording from the Release Face Membrane of Individual Functional Presynaptic Terminals

Published on: October 1, 2014

Related Experiment Videos

Last Updated: Jun 19, 2026

Modeling Biological Membranes with Circuit Boards and Measuring Electrical Signals in Axons: Student Laboratory Exercises
13:56

Modeling Biological Membranes with Circuit Boards and Measuring Electrical Signals in Axons: Student Laboratory Exercises

Published on: January 18, 2011

In Situ Visualization of Axon Growth and Growth Cone Dynamics in Acute Ex Vivo Embryonic Brain Slice Cultures
10:45

In Situ Visualization of Axon Growth and Growth Cone Dynamics in Acute Ex Vivo Embryonic Brain Slice Cultures

Published on: October 14, 2021

Acute Dissociation of Lamprey Reticulospinal Axons to Enable Recording from the Release Face Membrane of Individual Functional Presynaptic Terminals
12:01

Acute Dissociation of Lamprey Reticulospinal Axons to Enable Recording from the Release Face Membrane of Individual Functional Presynaptic Terminals

Published on: October 1, 2014

Area of Science:

  • Neuroscience
  • Biophysics
  • Electrical Engineering

Background:

  • Understanding neuronal membrane electrical properties is crucial for neuroscience.
  • Previous studies determined the dielectric characteristics of the squid giant axon membrane.

Purpose of the Study:

  • To investigate the longitudinal alternating current impedance of the squid giant axon.
  • To characterize the electrical properties of the neuronal membrane, including inductive components.

Main Methods:

  • Longitudinal alternating current impedance measurements were performed on squid giant axons.
  • Measurements spanned a frequency range from 30 Hz to 200 kHz.
  • Large seawater electrodes were used, with the inter-electrode length immersed in oil.

Main Results:

  • High-frequency impedance aligned with theoretical predictions based on membrane dielectric characteristics.
  • Axon impedance exhibited a maximum at low frequencies, with reactance vanishing between 150-300 Hz.
  • Inductive reactance was observed below this frequency, indicating an inductive structure within the axon membrane.

Conclusions:

  • The squid giant axon membrane possesses inductive properties.
  • An equivalent circuit model for the membrane includes inductance, capacitance, and resistance.
  • The membrane's capacity is 1 microfarad with dielectric loss, shunted by a series combination of 400 ohms resistance and 0.2 henry inductance per square centimeter.