How to Calculate Bending Shear Stress and Strength Condition of Beam?

There are both bending moment and shear force on the cross section of the beam with transverse force bending, so there are both normal stress and shear stress on the cross section.

Next, the bending shear stress of several common section beams is discussed.

Rectangular section

A micro segment with a length of dx is cut from the beam with transverse force bending.

There is no load on the beam, and the shear forces on both sides of the micro segment are equal, but the direction is opposite.

The bending moment on the right section has an increment relative to the left section.

Because the bending moments are different, the normal stress on the two sections is also different.

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For the narrow rectangular section, because there is no shear stress on the side of the beam, according to the shear stress reciprocity theorem, the shear stress at each point on both sides of the section is tangent to the boundary.

That is, parallel to the boundary, the beam is symmetrically bent, the shear stress on the y axis of the symmetry axis must be along the y direction, and the shear stress on the narrow section changes little along the width direction.

Therefore, the following assumptions are made about the distribution law of shear stress on the cross section:

  • The direction of shear stress at each point on the cross section is parallel to the shear force;
  • The shear stress is evenly distributed along the section width, that is, the shear stress at each point on the horizontal line parallel to the neutral axis is equal.

When the height width ratio of the section is greater than 2, the solution based on the above assumption has sufficient accuracy compared with the exact solution of the elastic theory.

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According to the reciprocal theorem of shear stress, there should be a shear stress equal to the size of the cross section on the longitudinal section perpendicular to the cross section.

Cut the micro segment along the longitudinal plane with the moment neutral wheelbase away from y, take the micro element on the lower side of the longitudinal plane, and the force is as shown in the figure below.

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The resultant force of normal stress on the left section is:

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The resultant force of normal stress on the right section is:

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Obviously, the two resultant forces are different in size.

There must be a force along the axial direction on the longitudinal section to keep the micro segment in balance.

This force is the resultant force of shear stress, which also proves that there is shear stress on the longitudinal section.

Since dx is a small amount, let the shear stress on the longitudinal plane be evenly distributed:

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According to equilibrium conditions:

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That is,

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Among,

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From the reciprocal theorem of shear stress and the differential relationship between shear force and bending moment:

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Of which:

  • b is the width of the horizontal line with the neutral axis of the moment y on the section, which is constant for rectangular sections;
  • Iz is the moment of inertia of the neutral axis of the entire cross-section;
  • Sz* is the static moment of the area outside the horizontal line whose neutral axis is y on the cross section to the neutral axis;
  • FS is the shear force on the cross section.

Among,

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Substitute into the formula of shear stress calculation

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The shear stress is parabola distributed along the section height.

When y=0, there is the maximum shear stress on the section at the neutral axis

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Angular strain is

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It can be seen that the angular strain is also parabola distributed along the section height.

At this time, the warping shape of the cross section when the cross force bends is shown in the figure below, which verifies that the cross force bending deformation does not meet the plane assumption.

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When the shear force is unchanged, the shear stress on the adjacent cross sections is the same, and the warpage degree is also the same.

The length of the longitudinal fiber will not change due to the warpage of the section, so it will not cause additional normal stress.

If the shear force changes with the position of the section, the warpage degree on the adjacent two sections is different, causing additional normal stress on the section.

For symmetrical sections of other shapes, the approximate solution of shear stress can be obtained according to the above derivation method.

For rectangular section, in the stress calculation formula, the section width b is constant, and the static moment of the half cross-sectional area on one side of the neutral axis to the neutral axis is the largest, so the shear stress at each point on the neutral axis is the largest.

For symmetrical sections of other shapes, the maximum shear stress on the cross section usually also occurs at various points on the neutral axis, except for sections with significantly increased width at the neutral axis (such as cross sections) or some sections with variable width (such as isosceles triangle sections).

Therefore, for I-shaped, annular and circular section beams, the maximum shear stress at each point on the neutral axis is mainly discussed below.

Circular section

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According to the reciprocal theorem of shear stress, the direction of shear stress at each point on the edge of the circular section is tangent to the circumference.

At each point of the axis of symmetry, the shear stress must follow the y direction.

Therefore, the distribution law of shear stress can be assumed as:

The shear stresses at each point along the width y from the neutral axis converge at a point on the axis of symmetry;

The components of shear stress along the Y direction at each point along the width are equal.

The maximum shear stress of the circular section is still on the neutral axis.

Since the direction of the shear stress at both ends of the neutral axis is tangent to the circumference and parallel to the action direction of the external force, the direction of the shear stress at each point on the neutral axis is parallel to the external force, and the value is equal.

The maximum shear stress is

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I-shaped cross-section

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The I-shaped section is an open thin-walled section, and the stress distribution is shown in the figure.

The magnitude of shear stress along the wall thickness is equal, which is called shear stress flow, and the flow direction is along the direction of shear (like water flow, along the direction of shear, from upstream to downstream).

The shear stress component parallel to the y-axis on the flange is secondary and neglected, mainly the shear stress component parallel to the long side of the flange.

The shear stress on the web is parabolic distribution, and the size of the stress is shown in the figure.

The maximum shear stress is at the neutral axis.

In case of I-shaped steel, the maximum shear stress:

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Where, b is the thickness of the web, and Iz/s*zmax can be obtained by referring to the profile steel table.

If it is an I-shaped section composed of three long and narrow rectangles, the maximum and minimum shear stresses on the web can be obtained as follows:

maximum and minimum shear stresses on the web

From the above two formulas, it can be seen that the width of the web is much smaller than the width of the flange, so the maximum shear stress on the web is not much different from the minimum shear stress.

Therefore, it can be considered that the shear stress on the web is roughly evenly distributed.

The resultant shear stress on the web accounts for 95-97% of the total shear force, and the shear force on the cross section is mostly borne by the web.

Since the web bears almost all the shear force on the section, and the shear stress on the web is nearly evenly distributed, the maximum shear stress can be approximately calculated by dividing the shear force by the cross-sectional area of the ventral pole:

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At the same time, the whole area of I-beam flange is farthest from the neutral axis, and the normal stress at each point is relatively large, so the flange bears most of the bending moment on the section.

Thin wall annular section

The thickness of thin-walled annular section is d, the average radius of the ring is r, and the thickness is far less than the average radius, so it can be assumed that:

The shear stress on the cross section is equal along the wall thickness;

The direction of shear stress is tangent to the central line of the section, and the direction of shear stress flow is along the shear direction.

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The maximum shear stress is located on the neutral axis:

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Where, A is the area of the annular section.

Strength condition of beam

Bending normal stress strength condition:

For neutral axisymmetric sections, the maximum tensile normal stress and the maximum compressive normal stress are equal.

Plastic materials are commonly used, and their strength conditions:

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As for the section with asymmetric neutral axis, the maximum tensile normal stress and the maximum compressive normal stress are not equal.

Brittle materials are commonly used, and their strength conditions:

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The strength condition of bending shear stress is:

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Measures to improve the bending strength of beams

Bending normal stress is the main factor controlling the beam.

Therefore, the strength condition of bending normal stress is often the main basis for the design of beams.

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From the strength condition, to improve the bearing capacity of the beam, two aspects should be considered:

On the one hand, the stress of the beam should be reasonably arranged to reduce the maximum bending moment;

On the other hand, reasonable section shape is adopted to improve the bending section coefficient of the section and make full use of the properties of the material.

1. Reasonably arrange the stress of the beam

Improve the stress condition of the beam and try to reduce the maximum bending moment in the beam.

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As shown in the fig., the maximum bending moment on the beam under uniform load is greatly reduced when the support is moved inward for a certain distance from the positions of both ends of the beam.

For example, the girder and cylindrical container of gantry crane, whose support point moves slightly to the middle, can achieve the effect of reducing the maximum bending moment.

2. Reasonable section of beam

The greater the flexural section coefficient, the smaller the stress and the higher the bearing capacity of the beam.

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For example, when the beam is loaded in the vertical direction, the bending section coefficient is larger when the section is placed vertically, so it is more reasonable to place it vertically than horizontally.

While improving the bending section coefficient of the section, we also hope to use less materials to achieve better economy.

Therefore, the ratio of bending section coefficient to section area is generally used to measure the rationality of section design.

Under the same cross-sectional area, rectangular section (height greater than width) is more reasonable than circular section, while I-shaped section or box section is more reasonable than rectangular section.

Therefore, in order to make full use of materials, materials should be placed as far away from the neutral axis as possible.

When discussing the reasonable shape of the section, the mechanical properties of the material should also be taken into account.

Materials with the same tensile and compressive strength (such as low carbon steel) should adopt neutral axisymmetric sections, such as circular, rectangular, I-shaped, box, etc.

In this way, the maximum tensile stress and the maximum compressive stress at the upper and lower edges of the section can be equal.

For materials with unequal tensile and compressive strengths (such as cast iron, cement, etc.), the section shape with the neutral axis inclined to the tensile side should be adopted.

Concept of equal strength beam

The beams discussed above are all of equal section, and the bending section coefficient is constant, but generally, the bending moment of each section of the beam changes with the position of the section.

The section design of equal straight beam should be carried out according to the maximum bending moment, and its maximum stress is close to the allowable stress.

The bending moment on other sections is small, so the stress is small, and the material is not fully utilized.

In order to save materials and reduce self weight, the section size can be changed so that the bending section coefficient changes with the bending moment.

A larger section is used where the bending moment is larger, while a smaller section is used where the bending moment is smaller.

This kind of beam whose section changes along the axis is called variable section beam.

If the maximum normal stress on each cross-section of a variable cross-section beam is equal and equal to the allowable stress, it is called an equal strength beam.

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