
An axial load is an external action applied along a structural member’s longitudinal axis. Axial force is the internal section force that develops as the structure resists that action. Engineers use these concepts to evaluate tension, compression, stress, buckling, and combined loading in beams, columns, braces, trusses, and FEA models.
An axial load is an external force applied along the longitudinal axis of a structural member. When the load acts through the centroid of the cross-section, it produces primarily axial tension or compression. If the load is applied eccentrically, the member is subjected to combined axial force and bending.
The force acts parallel to the member axis. In an ideal case, the load passes through the centroid of the cross-section, producing a uniform axial response.
Depending on its direction, an axial load can create:
For example, a hanging rod supporting a suspended load is subjected to tensile axial loading, while a building column carrying gravity loads experiences mostly compressive axial loading.
Axial loads are common in many structural applications, including columns, braces, truss members, tie rods, cables, bolts, and lifting structures.
Axial force is the internal force developed because of applied loads, support reactions, imposed displacements, temperature effects, restressing, constraints, and load transfer through connected members. Unlike an applied load, which acts on the structure from outside, axial force is the resultant internal normal force acting across a member cross-section and required to satisfy equilibrium. It acts along the longitudinal axis of the element and tends to either stretch the member (tension) or shorten it (compression).
In mechanics, these internal actions include normal (axial) forces, shear forces, bending moments, and torsional moments. Axial force, also referred to as a normal force, acts along the member to the examined cross-section and is responsible for tensile or compressive behavior.
Axial force is the internal force that develops within a structural member to resist an externally applied load. It acts along the member’s longitudinal axis and can occur in two forms:
The magnitude and sign of the axial force depend on the equilibrium of the member and the loads acting on it. Unlike axial load, which is an external action applied to a structure, axial force represents the internal force that exists within the member itself.
Image: Axial force illustration
In structural analysis and FEA software, axial force is commonly denoted by N. It is typically presented as an internal result for beam, frame, or truss elements and may be shown in force tables or axial force diagrams. Depending on the adopted sign convention, positive values often indicate tension and negative values indicate compression.
An axial load is an external action applied to a structure, while axial force is the internal response developed within a member to resist that loading. The final axial force value depends not only on the applied load itself but also on support conditions, constraints, and the behavior of the entire structural system.
| Term | Meaning | Where it appears |
| Axial load | External load applied along the member axis | Load cases, applied nodal or member loads, and model inputs |
| Axial force | Internal force developed inside the member | Member-force results, section cuts, tables, and force diagrams |
When a structural member is subjected to axial loading, the internal response appears as axial (normal) force, which can act in either tension or compression depending on the direction of loading and boundary conditions.
A tensile axial force occurs when the internal force tends to elongate the member. The material fibers are pulled apart, and the member is subjected to stretching along its longitudinal axis.
A compressive axial force occurs when the internal force tends to shorten the member. The material fibers are pushed together, and the member resists shortening along its axis.
The sign assigned to tensile and compressive forces depends on the adopted convention. Under the sign convention used in this example, tension is positive and compression is negative. Analysis software may use a different convention, particularly for element-end forces and internal force outputs, so engineers should always verify the solver documentation and element local axis orientation before interpreting results.
Both tensile and compression forces are structurally important, but they can lead to different failure mechanisms. Members subjected to tension typically fail when the material reaches its strength limit. For example, bolts and tie rods may fail under excessive tensile loading because they cannot buckle. Compression members, on the other hand, may fail either by material crushing or by buckling instability. Slender columns and braces are particularly sensitive, as small imperfections or load eccentricities can cause the member to lose stability and buckle before reaching its ultimate material strength.
The relationship between axial stress and axial force is commonly used to estimate the behavior of members subjected to pure axial loading. For a simple prismatic member with a uniform cross-section, axial stress can be calculated as:
σ = F / A
where:
The equation can also be rearranged to determine axial force:
\( N = \sigma_{\text{avg}} A \)
These equations assume that stress is evenly distributed across the cross-section and that the member is subjected to concentric axial loading. They provide the average normal stress in a simple member and are widely used in mechanics of materials. However, they do not determine axial force distribution in general frames, trusses, or FEA models, where internal forces are obtained through equilibrium equations and structural analysis.
Some common examples include:
An axial force diagram shows how internal axial force changes along the length of a structural member such as a beam, column, cable, or truss element.
The horizontal axis represents the position along the member, and the vertical axis represents the corresponding internal axial force. The diagram illustrates how axial force changes from one cross-section to another.
The sign of the force indicates the loading type:
The exact convention can vary depending on the software or design standard used.
For a straight one-dimensional member, the axial force remains constant between two points if there is no distributed axial load or other axial force transfer along that segment. These regions appear as horizontal segments in the diagram.
Sudden changes in the diagram occur at locations where concentrated loads or support reactions introduce an axial force component. The magnitude of the jump is equal to the component of the applied force acting along the member’s local axis.
Consider a straight bar fixed at one end and subjected to two axial point loads of 20 kN and 10 kN acting along its axis. From equilibrium, the support reaction is 30 kN.
To calculate the axial force, make section cuts between the loads and apply equilibrium equations to each segment:
This piecewise result can then be used to draw the axial force diagram. The diagram consists of three constant-force regions separated by abrupt jumps at the load application points. Each jump is equal to the magnitude of the corresponding axial point load.
If the first segment has a cross-sectional area of 1,000 mm², the average axial stress is:
σ = N/A = 30,000 N / 1,000 mm² = 30 MPa
Image: Axial force diagram example with support reactions and stress calculation
This axial force diagram example demonstrates how support reactions, section cuts, equilibrium equations, and the axial stress formula are used together to determine internal forces in a member under axial loading.
In Finite Element Analysis (FEA), axial force is a standard result output for beam, truss, and frame elements. However, interpreting axial-force results requires more than simply reading a single value from the postprocessor.
When reviewing axial force in FEA, engineers should consider:
Axial force should also be evaluated together with bending moments, shear forces, buckling effects, and code-based resistance checks. On its own, axial force rarely provides sufficient information for structural verification, particularly in members where combined loading governs the design.
The final axial force value depends not only on the individual loads included in a load combination but also on the load factors applied to each load case. As a result, different combinations and envelopes may produce significantly different governing axial forces in the same member.
A critical aspect in FEA interpretation is the element coordinate systems in FEA. For one-dimensional beam, frame, bar, and truss elements, axial force is typically reported along the element’s longitudinal local axis, which may be designated as local x, local 1, or another solver-specific axis. Misinterpreting the local axis orientation or sign convention can lead to incorrect conclusions about whether a member is in tension or compression.
For shell and solid elements, a single member-level axial force result is usually not available. Instead, engineers typically evaluate stresses, membrane-force resultants, section forces, or forces integrated across a section cut to assess axial loading effects.
Axial force must also be evaluated together with:
On its own, axial force does not provide sufficient information for structural verification, especially in members where combined loading governs design.
This is why many engineering teams use structural analysis and design software SDC Verifier. The software helps engineers use FEA results in a structured verification workflow. It can recognize structural details, organize load cases and combinations, perform code-based strength and stability checks, and generate reports that update with the calculation model.
The difference between axial and radial loads lies in the direction of force application relative to the member or component axis.
Image: Axial and radial loads acting on a bearing
| Term | Direction | Typical Effect |
| Axial load | Along the axis | Tension or compression |
| Radial load | Perpendicular to the axis | Bending or shear loading |
Focusing on a single axial force value without considering the broader structural context can lead to incorrect engineering conclusions.
Some common mistakes include:
An axial load is a force applied parallel to the longitudinal axis of a member. Depending on its direction, it places the member in either tension or compression.
Axial force is the internal force that acts along a member’s axis in response to external loading. It represents the tension or compression developed within the member.
An axial load refers to an external action applied along a member axis, while axial force refers to the internal section force that develops within the member. The terms are sometimes used interchangeably in less formal contexts, but they describe different roles in structural analysis.
There is no single universal formula for axial force in a complete structure. Axial force is typically determined from equilibrium equations or structural analysis. For a simple member with known average normal stress, the relationship is:
\( F = \sigma_{\text{avg}} A \)
where F is axial force, σ is axial stress, and A is the cross-sectional area.
An axial force diagram shows how the internal axial force changes along the position of a member. It helps identify regions subjected to tension or compression and locate critical force values.
The sign convention depends on the adopted standard or software. In many engineering applications, tension is considered positive and compression negative, but the opposite convention may also be used.
An axial load acts parallel to the axis of a member or component and produces tension or compression. A radial load acts perpendicular to the axis and typically introduces transverse forces and bending effects.
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