This page lists the cross section properties calculated by
ShapeDesigner Pro
software. These calculated section properties are listed here and presented in the table below:
mass, volume, cross section area, transformed composite cross section mass, volume and area,
moment of inertia, product of inertia, polar moment of inertia, radius of gyration,
position and orientation of the principal, neutral and plastic axis,
torsion constant, warping constant, sectorial product of area, elastic modulus,
plastic modulus, shape factor, centroid, shear center, fully plastic moment, maximum elastic moment,
shear constant, reduced shear areas, constants of stability, fully plastic torque and
flexural-torsional constant.
Calculated cross section properties
| Property |
Description |
| Mass |
mass |
| Volume |
volume |
| Area |
Cross section area |
| CMass |
Transformed composite cross section mass |
| CVolume |
Transformed composite cross section volume |
| CArea |
Transformed composite cross section area |
| Ixx, Iyy |
Moment of inertia about x and y axis |
| Ixy |
Product of inertia about origin |
| Io |
Polar moment of inertia about origin |
| rx, ry |
Radius of gyration about x and y axis |
| Ixp, Iyp |
Moment of inertia about principal x and y axis through centroid |
| Ixyp |
Product of inertia about centroid (principal direction) |
| rxp, ryp |
Radius of gyration about principal x an y axis through centroid |
| Iop |
Polar moment about origin of the centroidal principal axes |
| b |
Angle of orientation (direction) of the principal x axis |
| Imin, Imax |
Minimum and maximum magnitudes of principal moment of inertia |
| Ixc, Iyc |
Moment of inertia about x and y axis through centroid |
| rxc, ryc |
Radius of gyration about x and y axis through centroid |
| Ioc |
Polar moment of inertia about origin of the centroidal axes |
| J |
Torsion constant |
| Cw |
Warping constant |
| Swx, Swy |
Sectorial product of area with respect to x and y axis |
| Stx, Sbx |
Elastic modulus about x axis at top and bottom |
| Sty, Sby |
Elastic modulus about y axis at top and bottom |
| zx, zy |
Plastic modulus about x and y axis |
| fx, fy |
Shape factor in x and y (Plastic neutral) direction |
| O |
Angle of orientation of the neutral axis from principal x-axis |
| PNA |
Position of the plastic neutral axis |
| xc, yc |
X and y location of centroid |
| xs, ys |
X and y location of shear center |
| Mpmax |
Fully plastic moment |
| Memax |
Maximum elastic moment |
| kx, ky |
Section shear constant about x and y axis |
| ax, ay |
Reduced shear areas about x and y axis |
| bx, by |
Constants of stability |
| Tpmax |
Fully plastic torque |
| Dsc |
Distance between shear center and centroid |
| bft |
Flexural-torsional constant |
Maximum stresses
- sx: Axial stress
- sw: Axial warping stress
- tsx, tsy: Shear stress in x and y directions
- txz, tyz: Torsional shear stress in x and y directions
Minimum stresses
- sx: Axial stress
- sw: Axial warping stress
- tsx, tsy: Shear stress in x and y directions
- txz, tyz: Torsional shear stress in x and y directions
Stresses at custom position
- sx: Axial stress
- sw: Axial warping stress
- tsx, tsy: Shear stress in x and y directions
- txz, tyz: Torsional shear stress in x and y directions
- qx, qy: Flow stress in x and y directions
- sI: sII ; sIII: Principal stresses
Failure criteria for yield strength
- Maximum normal stress criterion
- Tresca criterion
- Von Mises-Hencky criterion
- Saint-Venant criterion
- Maximum strain energy criterion
ShapeDesignerPro Product Page
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ShapeDesigner Pro product page.
Real Time Property Display
ShapeDesigner displays all geometric properties in real time in the CAD at design time. This
means, for example, that you can move a point and see how the properties such as area or inertia
evolve as the movement is occurring.
Real Torsion and Warping Constants
Contrary to most software available, ShapeDesigner makes no assumptions or restrictions on the
calculation of shear and torsion properties. ShapeDesigner uses an advanced and efficient finite
element approach to calculate these constants. The complexity of the finite element approach is
hidden from the user. There is no general method for computing shear and torsion
properties without using this finite element approach.