Shape functions determine how each element’s interior displacement is reconstructed from its nodal displacement values. They provide the interpolation rule that connects discrete unknowns at nodes to a field inside the element, rather than assigning an independent value everywhere. This connection lets the mathematical model replace a continuous displacement field with a manageable set of nodal values for subsequent analysis.
A variational or weighted-residual formulation converts the governing requirements into equations for the unknown nodal values. Instead of demanding that equilibrium and boundary conditions hold point by point in the original continuous problem, it imposes them through an approximation over the modeled domain. This allows the final algebraic system to represent the governing behavior without reproducing the full field exactly.
Partitioning the domain localizes the interpolation process. Each element receives a relationship between its nodal values and the displacement represented within that element, while the collection of elements supplies the overall approximation. This organization makes a continuous boundary-value problem tractable as a finite system and provides the framework in which equilibrium and boundary conditions are imposed approximately.
An analysis first represents the domain as elements, identifies nodal displacement unknowns, and specifies the shape functions used within each element. The element-level relations are then combined into a finite set of equations, typically through a variational or weighted-residual formulation. Boundary conditions and equilibrium enter that formulation, and solving the resulting equations yields the nodal values used to describe the displacement field.
It is useful when a displacement field is governed by differential equations but cannot be handled conveniently in its continuous form. The method provides a finite-equation representation for boundary-value problems, making it applicable to elasticity and structural deformation. Its value lies in retaining the behavior needed for analysis while replacing an unknown field with a simpler, computationally manageable representation.
Because the formulation is tied to differential equations, equilibrium, and boundary conditions rather than to one particular application, the same strategy can be used across boundary-value problems. In the stated context, it supports elasticity and structural deformation; more generally, it offers a way to convert continuous field analysis into a finite set of equations while preserving the behavior relevant to the problem.