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 Experiment Video

Updated: Jan 9, 2026

Shock Wave Application to Cell Cultures
05:39

Shock Wave Application to Cell Cultures

Published on: April 8, 2014

13.2K

Nonlinear transmission line: Shock waves and the simple wave approximation.

Eugene Kogan1

  • 1Department of Physics, Bar-Ilan University, Ramat-Gan 52900, Israel.

Chaos (Woodbury, N.Y.)
|December 2, 2025
PubMed
Summary
This summary is machine-generated.

Related Concept Videos

Traveling Waves: Lossless Lines01:27

Traveling Waves: Lossless Lines

454
The provided content explores the behavior of traveling waves on single-phase lossless transmission lines. It begins with a single-phase two-wire lossless transmission line of length Δx, characterized by a loop inductance LH/m and a line-to-line capacitance C F/m. These parameters result in a series inductance LΔx  and a shunt capacitance CΔx.
454
Lossy Lines and Overvoltages01:22

Lossy Lines and Overvoltages

336
Transmission-line series resistance and shunt conductance cause three primary effects: attenuation, distortion, and power losses.
Attenuation
When constant series resistance and shunt conductance are present, voltage and current equations are modified. The propagation constant indicates that voltage and current waves consist of both forward and backward traveling components. These waves attenuate as they propagate, with the attenuation factor related to the resistance and conductance. In a...
336
Lossless Lines01:23

Lossless Lines

533
In electrical engineering, a lossless transmission line is characterized by a purely imaginary propagation constant and a resistive characteristic impedance. The ABCD parameters, which describe the relationship between the input and output voltages and currents, indicate an equivalent π circuit with an imaginary series impedance and a shunt admittance. This results in a transmission line that, when the product of the phase constant (beta) and the length of the line is less than pi, exhibits...
533
Linear Approximation in Frequency Domain01:26

Linear Approximation in Frequency Domain

332
Linear systems are characterized by two main properties: superposition and homogeneity. Superposition allows the response to multiple inputs to be the sum of the responses to each individual input. Homogeneity ensures that scaling an input by a scalar results in the response being scaled by the same scalar.
In contrast, nonlinear systems do not inherently possess these properties. However, for small deviations around an operating point, a nonlinear system can often be approximated as linear....
332
Boundary Conditions: Lossless Lines01:21

Boundary Conditions: Lossless Lines

398
Consider a single-phase, two-wire, lossless transmission line terminated by an impedance at the receiving end and a source with Thevenin voltage and impedance at the sending end. The line, with length, has a surge impedance and wave velocity determined by the line's inductance and capacitance.
At the receiving end, the boundary condition states that the voltage equals the product of the receiving-end impedance and current. This relationship is expressed as a function of the incident and...
398
Transmission-Line Differential Equations01:26

Transmission-Line Differential Equations

937
Transmission lines are essential components of electrical power systems. They are characterized by the distributed nature of resistance (R), inductance (L), and capacitance (C) per unit length. To analyze these lines, differential equations are employed to model the variations in voltage and current along the line.
Line Section Model
A circuit representing a line section of length Δx helps in understanding the transmission line parameters. The voltage V(x) and current i(x) are measured from...
937

You might also read

Related Articles

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

Sort by
Same author

Graphene for Electronics.

Nanomaterials (Basel, Switzerland)·2022
Same author

Screening in Graphene: Response to External Static Electric Field and an Image-Potential Problem.

Nanomaterials (Basel, Switzerland)·2021
Same journal

Multiscale dynamics of special memristive ion channels in a neural circuit.

Chaos (Woodbury, N.Y.)·2026
Same journal

Symmetry-protected delay spectroscopy in oscillator networks.

Chaos (Woodbury, N.Y.)·2026
Same journal

Mesoscale community organization governs epidemic onset and spread in metapopulations.

Chaos (Woodbury, N.Y.)·2026
Same journal

Topological dependence of viral mutation spread in complex host-interaction networks.

Chaos (Woodbury, N.Y.)·2026
Same journal

Multifractal signatures of Hamiltonian chaos in Hyperion's rotational dynamics.

Chaos (Woodbury, N.Y.)·2026
Same journal

Exploring mechanisms for reversal of flow in tunicate hearts.

Chaos (Woodbury, N.Y.)·2026
See all related articles

This study analyzes nonlinear transmission lines with and without dissipation. Researchers found analytic solutions for shock wave profiles in dissipative lines and described wave formation in lossless lines using a simple wave approximation.

Area of Science:

  • Nonlinear dynamics
  • Electrical engineering
  • Wave propagation

Background:

  • Transmission lines are fundamental components in electrical systems.
  • Nonlinear elements introduce complex wave behaviors.
  • Dissipation significantly impacts wave characteristics.

Purpose of the Study:

  • To investigate shock wave phenomena in nonlinear transmission lines.
  • To analyze the effects of linear ohmic resistors (dissipation) on wave propagation.
  • To develop approximations for describing wave formation in both lossy and lossless lines.

Main Methods:

  • Mathematical modeling of nonlinear transmission lines with nonlinear inductors and capacitors.
  • Inclusion of linear ohmic resistors to account for dissipation.

More Related Videos

An Analog Macroscopic Technique for Studying Molecular Hydrodynamic Processes in Dense Gases and Liquids
11:03

An Analog Macroscopic Technique for Studying Molecular Hydrodynamic Processes in Dense Gases and Liquids

Published on: December 4, 2017

8.9K
Transmission of Multiple Signals through an Optical Fiber Using Wavefront Shaping
09:43

Transmission of Multiple Signals through an Optical Fiber Using Wavefront Shaping

Published on: March 20, 2017

10.3K

Related Experiment Videos

Last Updated: Jan 9, 2026

Shock Wave Application to Cell Cultures
05:39

Shock Wave Application to Cell Cultures

Published on: April 8, 2014

13.2K
An Analog Macroscopic Technique for Studying Molecular Hydrodynamic Processes in Dense Gases and Liquids
11:03

An Analog Macroscopic Technique for Studying Molecular Hydrodynamic Processes in Dense Gases and Liquids

Published on: December 4, 2017

8.9K
Transmission of Multiple Signals through an Optical Fiber Using Wavefront Shaping
09:43

Transmission of Multiple Signals through an Optical Fiber Using Wavefront Shaping

Published on: March 20, 2017

10.3K
  • Derivation of analytic solutions for strong dissipation cases.
  • Formulation of a simple wave approximation for lossless lines.
  • Main Results:

    • Existence of shock waves (traveling waves with distinct pre- and post-wave front values) due to dissipation.
    • Analytic solution for shock wave profiles under strong dissipation.
    • Identification of stationary dispersive shock waves in weakly dissipative lines.
    • The simple wave approximation effectively describes shock wave formation in lossy lines.

    Conclusions:

    • Dissipation in nonlinear transmission lines leads to shock wave formation.
    • Analytic solutions are achievable for specific dissipation levels.
    • The simple wave approximation provides a valuable tool for understanding wave dynamics in these systems.