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Angle of Twist: Problem Solving01:13

Angle of Twist: Problem Solving

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An electric motor applies a torque of 700 N·m to an aluminum shaft, triggering a stable rotation. Two pulleys, B and C, are subjected to torques of 300 N·m and 400 N·m, respectively. The modulus of rigidity is provided as 25 GPa. With the knowledge of the length and diameter of each segment, the twist angle between the two pulleys can be computed. First, a section cut is made between pulleys B and C, and the cut cross-section is analyzed using a free-body diagram. Given that the torque...
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Bending01:10

Bending

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Pure bending is a fundamental concept in structural mechanics, essential for understanding how materials deform under symmetrical loads without direct forces. Pure bending occurs when prismatic members, such as beams, are subjected to equal and opposite moments that induce bending. The phenomenon is crucial as it allows for predicting stress distributions without the influence of axial or shear forces.
In pure bending, the bending stress in a beam is calculated based on the bending moment and...
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Symmetric Member in Bending01:07

Symmetric Member in Bending

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In the study of the mechanics of materials, analyzing the behavior of prismatic members under opposing couples is crucial for understanding internal stress distributions, which are essential for structural design. When subjected to couples, a prismatic member experiences internal forces that maintain equilibrium. A couple, characterized by two equal and opposite forces, creates a moment but no resultant force. The internal forces at any section cut of the member must balance these external...
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Unsymmetric Bending01:18

Unsymmetric Bending

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Unsymmetrical bending occurs when the bending moment applied to a structural member does not align with its principal axis. This misalignment leads to complex stress distributions and deflection patterns that differ from those in symmetrical bending, and are essential for designing structures to withstand different loading conditions. In unsymmetrical bending, the neutral axis—where stress is zero—does not necessarily align with the geometric axes of the cross-section. The...
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Angle of Twist - Elastic Range01:13

Angle of Twist - Elastic Range

808
Consider a cylindrical shaft with a length denoted by L and a consistent cross-sectional radius referred to as r. This shaft undergoes a torque at the free end. The highest shearing strain within the shaft is directly proportional to the twist angle and the radial distance from the shaft axis. When the shaft behaves elastically, this shearing strain can be articulated using variables such as the applied torque, radial distance, the polar moment of inertia, and the modulus of rigidity. By...
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Work Done on a System by External Force01:11

Work Done on a System by External Force

3.0K
The work done by an external force on a particle changes its kinetic energy. However, internal forces must also be considered for a system of interacting particles. The potential energy formulation helps formulate the effect of internal forces. The net work done by an external force can be written in terms of the total change of mechanical energy, which includes both kinetic and potential energies.
In the presence of a non-conservative opposing force, like friction, some part of the work done...
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Related Experiment Video

Updated: Feb 4, 2026

High-Contrast and Fast Photorheological Switching of a Twist-Bend Nematic Liquid Crystal
06:24

High-Contrast and Fast Photorheological Switching of a Twist-Bend Nematic Liquid Crystal

Published on: October 31, 2019

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Nematic twist-bend phase in an external field.

Grzegorz Pająk1,2, Lech Longa1, Agnieszka Chrzanowska3

  • 1Marian Smoluchowski Institute of Physics, Department of Statistical Physics, Jagiellonian University, 30-348 Kraków, Poland; grzegorz@th.if.uj.edu.pl lech.longa@uj.edu.pl achrzano@usk.pk.edu.pl.

Proceedings of the National Academy of Sciences of the United States of America
|October 13, 2018
PubMed
Summary

Applied fields induce rich structural changes in the nematic twist-bend phase. Depending on permittivity, this liquid crystal can transition to uniaxial, elliptical, or splay-bend nematic phases, eventually forming polar structures.

Keywords:
chiralitynematicspolaritysplay–bendtwist–bend

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Area of Science:

  • Liquid crystal physics
  • Soft matter theory
  • Materials science

Background:

  • The nematic twist-bend phase exhibits unique structural properties relevant to mirror symmetry breaking.
  • Understanding its response to external fields is crucial for fundamental insights into liquid crystal behavior.

Purpose of the Study:

  • To theoretically investigate the structural transformations and stability of the nematic twist-bend phase under an applied uniform electric field.
  • To elucidate the mechanisms driving these field-induced phase transitions.

Main Methods:

  • Utilized Landau-de Gennes theory to model the nematic twist-bend phase.
  • Analyzed the effects of varying electric field strengths on the phase's structural properties and stability.
  • Considered systems with both positive and negative dielectric anisotropy.

Main Results:

  • For positive dielectric anisotropy, the phase transitions to a prolate uniaxial nematic phase, developing perpendicular polarization at high fields.
  • For negative dielectric anisotropy, new modulated structures emerge, including elliptical and splay-bend nematic phases.
  • Increasing fields lead to phase transitions into globally polar structures, including a chiral modification and a polar nematic phase.

Conclusions:

  • The nematic twist-bend phase exhibits complex field-dependent structural polymorphism.
  • Applied fields can induce transitions from nonpolar to polar states, offering insights into chirality and symmetry breaking in achiral systems.
  • The theoretical framework provides a basis for understanding and potentially controlling liquid crystal phases with external stimuli.