Any interaction that will change the motion, direction or structure of an object is considered a force.

A force can cause an object with mass to accelerate, to deform, or to accelerate and deform simultaneously.

A force is a vector quantity, with magnitude and direction, and it can be measured in the SI unit of Newtons. t is usually represented by the symbol F.

The magnitude of a force can be calculated as the product of the object’s mass and acceleration.

When not applied on an axial direction, a force can cause twisting or bending. These twisting and bending forces are referred to as moments. At a specific point, the moment caused by a force is equal to the product of the force’s magnitude and the distance between the point studied and the point where the force is applied.

A force can cause an object with mass to accelerate, to deform, or to accelerate and deform simultaneously.

A force is a vector quantity, with magnitude and direction, and it can be measured in the SI unit of Newtons. t is usually represented by the symbol F.

The magnitude of a force can be calculated as the product of the object’s mass and acceleration.

When not applied on an axial direction, a force can cause twisting or bending. These twisting and bending forces are referred to as moments. At a specific point, the moment caused by a force is equal to the product of the force’s magnitude and the distance between the point studied and the point where the force is applied.

In solid mechanics, the external forces acting on a structure and causing deformation or damage are defined as loads.

To ensure safety of a designed product, the loads expected to act on the product must be defined for analysis.

Loads can be categorized into static and dynamic loads depending on whether they change over time or not. The own weight of a structure is an example of static load. Impact loads caused by sudden acceleration or deceleration of equipment, or a motor spinning at a certain rpm, are categorized as dynamic loads.

The main loads used in analysis are the own weight of the structure, dead and live loads, pressure loads, temperature loads, wind, seismic loads, and vibrational and impact loads.

To ensure safety of a designed product, the loads expected to act on the product must be defined for analysis.

Loads can be categorized into static and dynamic loads depending on whether they change over time or not. The own weight of a structure is an example of static load. Impact loads caused by sudden acceleration or deceleration of equipment, or a motor spinning at a certain rpm, are categorized as dynamic loads.

The main loads used in analysis are the own weight of the structure, dead and live loads, pressure loads, temperature loads, wind, seismic loads, and vibrational and impact loads.

The third of Newton’s Laws of Motion states that all forces occur in pairs such that if one object exerts a force on another object, the second object will exert an equal and opposite reaction force on the first.

In general, reaction forces appear at the point of constraint, and in the direction in which the motion of the structure is restricted.

The sum of external forces, or loads, and the sum of reaction forces have the same value, but act in opposite direction.

Reaction forces are used as important data in the design of supports.

Since loads and reaction forces have the same value and act in opposite direction, the overall structure has no motion. Therefore, if a cut is made at any point in a structure, the resulting parts should also have no motion. The forces acting within the cut cross section are defined as internal forces.

In accordance with Newton’s Third Law of Motion, the sum of loads and reaction forces on each cut part and the sum of internal forces on that part have the same value.

Generally, internal forces divided by cross section are defined as stress.

Generally, internal forces divided by cross section are defined as stress.

Stress refers to the internal force per unit area. It is mathematically expressed by the following equation, where F is the force and A the area:

Since internal force is a vector having a magnitude and direction, stress is also defined as a vector physical quantity.

The stress acting on a face placed in any direction can be divided into components acting parallel and perpendicular to the face.

Normal stress is the stress acting in a direction perpendicular to a face.

Shear stress is the stress acting in a direction parallel to a face.

The stress acting on a face placed in any direction can be divided into components acting parallel and perpendicular to the face.

Normal stress is the stress acting in a direction perpendicular to a face.

Shear stress is the stress acting in a direction parallel to a face.

Changes in the spatial position of a structure are collectively defined as displacement.

Displacement is not necessarily accompanied by deformation; a representative example would be rigid body motion.

Rigid body motion is a type of behavior wherein the position of an object in space changes through translation and rotation only, with no change in the relative distance between two points in the object.

Displacement is not necessarily accompanied by deformation; a representative example would be rigid body motion.

Rigid body motion is a type of behavior wherein the position of an object in space changes through translation and rotation only, with no change in the relative distance between two points in the object.

Deformation refers to a change in the external shape of a structure.

When deformation occurs, all points within an object, or all points except for some points, are displaced, and the relative distance between two points changes.

When deformation occurs, all points within an object, or all points except for some points, are displaced, and the relative distance between two points changes.

Strain is categorized into normal strain and shear strain, and it is a dimensionless quantity.

Normal strain expresses the degree by which an object stretches or shrinks in a certain direction. It is mathematically defined as the increase in length in the axial direction of an object (a+b) divided by the original length of such object (l). It can be expressed in the form of this equation:

Normal strain expresses the degree by which an object stretches or shrinks in a certain direction. It is mathematically defined as the increase in length in the axial direction of an object (a+b) divided by the original length of such object (l). It can be expressed in the form of this equation:

Shear strain expresses the degree to which an object is crushed. It is defined as the change in angle, measured in radians, between two edges that form a right angle:

The stress-deformation rate relationship is the most important characteristic in defining the dynamic behavior of a material. It can be defined through the tensile testing of the material.

If the stress is plotted against the deformation, the graph would look like this:

The zone wherein the material returns to its original shape after the acting load has been removed is defined as the elastic zone of the material. In this zone, stress and deformation have a linear proportional relationship. The value of the slope in such linear relationship is called the elastic modulus (E), and the relationship between stress and deformation can then be expressed as:

The zone wherein the material cannot return to its original shape even after the acting load has been removed is defined as the plastic zone. Here, it is said that permanent deformation has occurred and that the material has yielded.

The boundary between the elastic and plastic zones is called the yield point. The stress at this point is defined as the yield stress.

The value of the stress at the point where fracture starts to occur is referred to as the ultimate stress.

The value of the stress at the point where fracture starts to occur is referred to as the ultimate stress.

The ultimate purpose of solid mechanics is finding out how much deformation occurs in a designed product depending on its shape and its material characteristics.

Therefore, if the deformation (δ) caused by a load (P) can be calculated using the area (A), the original length (L) and the elastic modulus (E), such deformation value can then be used to calculate the strain (ε). From the strain, the stress (σ) is then computed.

- Young’s Modulus or Modulus of Elasticity
- Poisson’s Ratio
- Density (when considering the effect of gravity and/or centrifugal loading)
- Coefficient of Thermal Expansion (when considering thermal loading)
- Shear Modulus (usually calculated from the Young’s Modulus and the Poisson’s Ratio)

- Adequate restraints to prevent rigid body motion

- Concentrated Forces
- Pressure
- Prescribed Nonzero Displacements
- Body Forces (gravitational and/or centrifugal)
- Thermal (temperature or temperature profile)