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

Stability of structures01:14

Stability of structures

377
In mechanical engineering, the stability of systems under various forces is critical for designing durable and efficient structures. One fundamental way to explore these concepts is by analyzing systems like two rods connected at a pivot point, O, with a torsional spring of spring constant k at the pivot point. This system is similar in appearance to a scissor jack used to change tires on a car. In this case, the arms of the linkage (equivalent to the rods in this system) are entirely vertical,...
377
Deformation in a Circular Shaft01:10

Deformation in a Circular Shaft

726
One of the distinctive characteristics of circular shafts is their ability to maintain their cross-sectional integrity under torsion. In other words, each cross-section continues to exist as a flat, unaltered entity, simply rotating like a solid, rigid slab. To understand the distribution of shearing stress within such a shaft, consider a cylindrical section inside this circular shaft. This section has a length of L and a radius of R, with one end fixed. The radius of the cylindrical section is...
726
Torsion of Noncircular Members01:16

Torsion of Noncircular Members

403
Circular shafts undergoing torsional stress maintain their cross-sectional integrity due to their axisymmetric nature. This symmetry ensures an even distribution of stress, allowing the shaft to withstand torsion without distorting. In contrast, square bars, lacking this axial symmetry, experience significant distortion across their cross-sections when subjected to torsion, with the exception of along their diagonals and at lines connecting midpoints. A detailed examination of a cubic element...
403
Statically Indeterminate Problem Solving01:16

Statically Indeterminate Problem Solving

609
Statically indeterminate problems are those where statics alone can not determine the internal forces or reactions. Consider a structure comprising two cylindrical rods made of steel and brass. These rods are joined at point B and restrained by rigid supports at points A and C. Now, the reactions at points A and C and the deflection at point B are to be determined. This rod structure is classified as statically indeterminate as the structure has more supports than are necessary for maintaining...
609
Temperature Dependent Deformation01:12

Temperature Dependent Deformation

298
In a nonhomogeneous rod made up of steel and brass, restrained at both ends and subjected to a temperature change, several steps are involved in calculating the stress and compressive load. Due to the problem's static indeterminacy, one end support is disconnected, allowing the rod to experience the temperature change freely. Next, an unknown force is applied at the free end, triggering deformations in the rod's steel and brass portions. These deformations are then calculated and added...
298
Deformations in a Symmetric Member in Bending01:18

Deformations in a Symmetric Member in Bending

396
When analyzing the deformation of a symmetric prismatic member subjected to bending by equal and opposite couples, it becomes clear that as the member bends, the originally straight lines on its wider faces curve into circular arcs, with a constant radius centered at a point known as Point C. This phenomenon helps to understand the stress and strain distribution within the member more clearly.
When the member is segmented into tiny cubic elements, it is observed that the primary stress...
396

You might also read

Related Articles

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

Sort by
Same author

Modeling Hemodynamics in Three-Dimensional, Biomimetic, Branched, Microfluidic, Vascular Networks.

Microcirculation (New York, N.Y. : 1994)·2024
Same author

When Is a Helix Stable?

Physical review letters·2020
Same author

Controlling sensation intensity for electrotactile stimulation in human-machine interfaces.

Science robotics·2019
Same author

Publisher Correction: Large-area MRI-compatible epidermal electronic interfaces for prosthetic control and cognitive monitoring.

Nature biomedical engineering·2019
Same author

Publisher Correction: Large-area MRI-compatible epidermal electronic interfaces for prosthetic control and cognitive monitoring.

Nature biomedical engineering·2019
Same author

Large-area MRI-compatible epidermal electronic interfaces for prosthetic control and cognitive monitoring.

Nature biomedical engineering·2019

Related Experiment Video

Updated: Dec 8, 2025

Flexural Rigidity Measurements of Biopolymers Using Gliding Assays
07:55

Flexural Rigidity Measurements of Biopolymers Using Gliding Assays

Published on: November 9, 2012

11.1K

Infinitely long isotropic Kirchhoff rods with helical centerlines cannot be stable.

Andy Borum1, Timothy Bretl2

  • 1Department of Mathematics, Cornell University, Ithaca, New York 14853, USA.

Physical Review. E
|September 18, 2020
PubMed
Summary

Planar elastic rods with constant curvature are always stable. However, nonplanar helical rods become unstable at a finite length, with critical length depending on curvature, torsion, and twist.

More Related Videos

Magnetically Induced Rotating Rayleigh-Taylor Instability
06:42

Magnetically Induced Rotating Rayleigh-Taylor Instability

Published on: March 3, 2017

9.9K
Finite Element Modeling for the Simulation of the Quasi-Static Compression of Corrugated Tapered Tubes
06:34

Finite Element Modeling for the Simulation of the Quasi-Static Compression of Corrugated Tapered Tubes

Published on: January 6, 2023

2.7K

Related Experiment Videos

Last Updated: Dec 8, 2025

Flexural Rigidity Measurements of Biopolymers Using Gliding Assays
07:55

Flexural Rigidity Measurements of Biopolymers Using Gliding Assays

Published on: November 9, 2012

11.1K
Magnetically Induced Rotating Rayleigh-Taylor Instability
06:42

Magnetically Induced Rotating Rayleigh-Taylor Instability

Published on: March 3, 2017

9.9K
Finite Element Modeling for the Simulation of the Quasi-Static Compression of Corrugated Tapered Tubes
06:34

Finite Element Modeling for the Simulation of the Quasi-Static Compression of Corrugated Tapered Tubes

Published on: January 6, 2023

2.7K

Area of Science:

  • Solid Mechanics
  • Elasticity Theory
  • Optimal Control

Background:

  • Planar elastic rods with constant curvature and clamped ends are known to be stable regardless of length.
  • The stability of nonplanar elastic rods, particularly helical configurations, remains less understood.

Purpose of the Study:

  • To investigate the stability of nonplanar elastic rods with helical centerlines.
  • To determine if helical rods with constant nonzero curvature can maintain stable equilibrium at any length.

Main Methods:

  • Application of optimal control theory to analyze the stability of Kirchhoff rods.
  • Derivation of coordinates for critical length computation, independent of stiffness parameters.
  • Development of a scaling relationship for instability length.

Main Results:

  • Demonstration that nonplanar helical rods with constant nonzero curvature become unstable at a finite length.
  • Identification of a critical length independent of bending and torsional stiffness.
  • Establishment of a scaling law linking instability length to curvature, torsion, and twist.

Conclusions:

  • Unlike their planar counterparts, nonplanar helical rods are not universally stable.
  • The derived critical length and scaling relationship provide key insights into the stability limits of helical elastic rods.