The capability to model piezoresistive effect exists in the following elements:
| PLANE222 - 2D 4-Node Coupled-Field Solid | 
| PLANE223 - 2D 8-Node Coupled-Field Solid | 
| SOLID225 - 3D 8-Node Coupled-Field Solid | 
| SOLID226 - 3D 20-Node Coupled-Field Solid | 
| SOLID227 - 3D 10-Node Coupled-Field Solid | 
In piezoresistive materials, stress or strain cause a change of electric resistivity:
(10–102)  | 
where:
| 
                     | 
| 
                     | 
| 
                     | 
| 
                     | 
| 
                     | 
(10–103)  | 
where:
| {r} = vector of matrix [r] components = [rx ry rz rxy ryz rxz]T | 
| 
                     | 
| 
                     | 
Similarly, for strains:
(10–104)  | 
where:
[m] = piezoresistive strain matrix (input on TB,PZRS
                    command with TBOPT = 1) | 
| {εel} = elastic strain vector | 
The coupled-field finite element matrix equation for the piezoresistive analysis is given by:
(10–105)  | 
The terms used in the above equation are explained in Piezoresistive Analysis where the conductivity matrix [Kv] is derived as:
(10–106)  |