Name: plane stress changes with rotation
Uploaded: 2025-05-22T09:06:18.000Z
Duration: 1 min 18 s
Channel: JoVE

Considere un punto de un cubo que experimenta una tensión plana, definida por sus componentes de tensión.
Si el elemento gira en ángulo, sus componentes de tensión cambian. Este cambio se determina considerando un elemento prismático con caras perpendiculares a sus ejes.
Al considerar el área de la cara oblicua, las áreas de las caras vertical y horizontal se pueden calcular utilizando funciones trigonométricas del ángulo de rotación.
Las fuerzas ejercidas sobre estas caras están representadas, y se supone que no actúan fuerzas sobre las caras triangulares del elemento. A continuación, las ecuaciones de equilibrio se escriben utilizando componentes a lo largo de los ejes girados.
Al resolver estas ecuaciones, se derivan los esfuerzos normal y cortante. A continuación, las tensiones normal y cortante se reexpresan mediante relaciones trigonométricas.
Una expresión para la tensión normal en el eje vertical girado se obtiene sustituyendo el ángulo de rotación en una de las expresiones anteriores por un nuevo ángulo.
Se observa que la suma de las tensiones normales ejercidas sobre un elemento cúbico permanece independiente de la orientación del elemento.

transformación de la tensión plana

<div>
 Estudiar la transformación de la tensión es esencial para comprender cómo los componentes de la tensión dentro de un material, como un cubo bajo tensión plana, cambian con la rotación. Este cambio se analiza considerando un elemento prismático dentro del cubo. A medida que el elemento gira, los componentes de tensión que actúan sobre él (tanto tensiones normales como cortantes) cambian en magnitud y orientación. Este cambio se cuantifica utilizando funciones trigonométricas del ángulo de rotación, relacionando las fuerzas que actúan sobre las caras del elemento girado con aquellas sobre sus caras perpendiculares originales.
 
 Las ecuaciones de equilibrio, formuladas considerando sólo las fuerzas sobre las caras perpendiculares a los ejes principales (excluyendo cualquier fuerza sobre las caras triangulares debida a la rotación), permiten derivar nuevos componentes de tensión. Las tensiones normales y cortantes se reexpresan en términos de las tensiones originales.
 
 <img alt="Equation 1" src="/files/ftp_upload/15652/15652_Equation_1.svg" style="text-align: center; height: 96px;">
 Se obtiene una nueva expresión para la tensión normal en el eje vertical girado reemplazando el ángulo de rotación en una expresión anterior por una nueva.
 
 <img alt="Equation 2" src="/files/ftp_upload/15652/15652_Equation_2.svg" style="text-align: center; height: 122px;">
 Un resultado notable de este análisis es que la suma de las tensiones normales no cambia independientemente de la orientación del elemento cúbico. Esta invariancia resalta la respuesta isotrópica del material a tensiones externas y es crucial para predecir el comportamiento del material bajo diferentes condiciones de carga. Comprender cómo se transforman los componentes de tensión con la orientación de los elementos es vital para predecir los modos de falla del material y diseñar materiales y estructuras que sean más resistentes a las cargas aplicadas.
 
</div>

Transformación de la tensión plana

Considere un punto de un cubo que experimenta una tensión plana, definida por sus componentes de tensión.
Si el elemento gira en ángulo, sus componentes de tensión cambian. ...

Education

Educación

JoVE Core

Mechanical Engineering

Ingeniería Mecánica

Unit 1

Unidad 1

Transformations of Stress and Strain

Transformaciones de esfuerzo y deformación

KEY TERMS AND CONCEPTS

TÉRMINOS Y CONCEPTOS CLAVE

Transformation of Plane Stress

plane stress changes with rotation

Plane stress changes with rotation in a material element. The analysis looks at a prismatic element inside a cube under plane stress. As the element turns, the normal stress and shearing stress on its faces change in both size and direction.

These changes are described with trigonometric functions of the rotation angle. The forces on the rotated faces are compared with the forces on the original faces that are perpendicular to each principal axis. The equilibrium equations use only the forces on those perpendicular faces, not the forces on the triangular faces created by the rotation.

From this balance, the new stress components can be written in terms of the original stresses. The normal stress on the rotated vertical axis is also found by using a new angle in a previous expression. One important result is that the sum of the normal stresses stays the same, no matter how the cubic element is oriented.

This invariant sum shows the material’s isotropic response to external stress. It helps explain how stress components shift as orientation changes. That understanding is important for predicting failure modes and for designing materials and structures that can better handle applied loads.

Plane Stress Changes with Rotation

transformation of plane stress

Plane stress changes with rotation in a material element. The analysis looks at a prismatic element inside a cube under plane stress. As the element turns, the normal stress and shearing stress on its faces change in both size and direction. These changes are described with trigonometric functions of the rotation angle. The forces on the rotated faces are compared with the forces on the original faces that are perpendicular to each principal axis. The equilibrium equations use only the forces...

principal stresses

Stress Circle for Principal and Shear Stress

The stress circle shows how normal stress and shearing stress change with angle on a transformed plane. Its center, C, lies on the vertical axis and represents the average normal stress. The radius shows the amount of stress variation as the plane rotates. Points A and B, where the circle crosses the horizontal axis, mark the maximum and minimum normal stresses. At these points, shearing stress is zero. These points define the principal stress planes, where only normal stress, called principal...

principal stresses: problem solving

Finding Principal Planes and Stress Limits

Principal planes and principal stresses are found by analyzing two planes that meet at right angles under shearing, tensile, and compressive stresses. The goal is to use the given stress values to describe how the material is loaded and to locate the planes where the stress state changes. To find the principal planes, use the formula that relates the plane angle to twice the shearing stress divided by the difference between tensile and compressive stresses. After substituting the known stress...

mohr&#39;s circle for plane stress

Reading Stress Components with Mohr's Circle

Mohr's circle is a graphical way to read the stress state at a point in a material under plane stress. It turns normal stress and shearing stress into a two-dimensional picture. This makes stress transformation easier to analyze. The method uses Cartesian coordinates. The horizontal axis shows normal stress, written as σ, and the vertical axis shows shearing stress, written as τ. Two points, A and B, are plotted from the stresses on the element. Point A is at (σx, -τxy), and point B is at (σx,...

general state of stress

Stress Tensor and Principal Stresses

The stress tensor describes the internal forces inside a material. It is used when a material is under external force or deformation. At a point such as O, the tensor can show the stress components on any plane through that point. A tetrahedral element helps show how these forces act. One face, XYZ, is perpendicular to the line OA. The other faces line up with the coordinate axes, and point O is the origin. The stress on the tetrahedron is split into normal and shear components on each face. <br...

yield criteria for ductile materials under plane stress

yield-criteria-for-ductile-materials-under-plane-stress

Tresca and Von Mises Yield Criteria

Ductile materials can yield when they are loaded beyond a safe stress level. Engineers use yield criteria to check whether structural elements and machine parts can handle the expected load without permanent deformation. The yield point is first found with a tensile test, which measures how the material responds to uniaxial stress. A tensile test is not enough when a part faces biaxial or plane stress conditions. In those cases, more advanced criteria are needed to predict failure. One common...

transformation of plane strain

Plane Strain Under Rotated Axes

Plane strain changes when the coordinate axes are rotated. This matters for long bars and similar elongated structures that are loaded uniformly on their sides. In these members, one dimension is much larger than the others, so deformation is mainly studied in a single plane. At a point such as O, the key strain components lie along the x and y axes. The strain along the z-axis is negligible in plane strain. Together, the x and y strain components describe the deformation state in the xy-plane.

mohr&#39;s circle for plane strain

Principal and Shear Strains on Mohr’s Circle

Mohr’s circle for plane strain shows how normal strain and shear strain change on a graph. The horizontal axis is normal strain, written as ε, and the vertical axis is shear strain, written as γ. It uses two plotted points, X and Y, to represent the strain state. Point X has coordinates (εx, -γXY), and point Y has coordinates (εY, γXY). The center of the circle, O, gives the average normal strain. The radius comes from the relationship between normal strain and shear strain, so the circle...

three-dimensional analysis of strain

Principal Strain Directions in 3D

Three-dimensional strain analysis shows how a material changes shape when it is loaded. It is especially useful for elastic, homogeneous materials. A small cubic element inside the material can expand or contract along principal stress axes. That change turns the cube into a rectangular parallelepiped, which makes the deformation easier to picture. The principal stress axes are orthogonal, or at right angles to each other. Along these directions, the stress does not create shear inside the...

measurements of strain

How Strain Gauges Measure Deformation

Strain describes how a material deforms when a force is applied. Normal strain compares the change in length with the original length. Engineers use this measure to track stretching or compression in materials. For higher accuracy, they often use electrical strain gauges. A strain gauge has a conductive wire on a paper backing that sticks to the surface of the material. It works through the piezoresistive effect, which means the wire’s electrical resistance changes when the material is bent,...

key terms and concepts

See how normal and shearing stress change as a plane-stressed element rotates, and why the sum of normal stresses stays constant for any orientation.

Plane Stress Changes with Rotation | JoVE K12

JoVE Core Mechanical Engineering offers concise, easy-to-understand animated videos covering key topics such as equilibrium, forces, truss analysis, and structural mechanics. Explore their real-world applications, and witness these concepts in action through scientist-led experiments.

mechanical engineering

Plane Stress Changes with Rotation

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