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A Biotensegrity Explanation for Structural Dysfunction in the Pelvis In Biotensegrity modeling of the pelvis, the expanded octahedron tensegrity (as in the logo above) is a useful starting point. Because it is oriented along the fa- miliar ‘x, y, and z’ axis’ it is easy to sche- matize the pelvis which has equivalent orientations (left/right, top/bottom, front/ back). Also this tensegrity has a central ‘cavity’ which expands or contracts and distorts, as forces are applied - a close analogy to the pelvic structure. This basic shape has been expanded to include the femurs and suggest the lower spine which is suspended and stabilized in the ten- sional network. The horizontal struts (x, and z axis’) illustrate the essential bal- ance of the ilia in relationship to the spine and femurs which are represented by the vertical (y axis) struts. biotensegrity modeling 1.5 © 2005 intension designs ltd. front view front view - distorted side view - distorted 3/4 view - normal 3/4 view - distorted top view top view - distorted side view Single Tensioned Pelvis model 05-STP-3.1 Pathomechanics of the pelvis and lower back can be illustrated by shortening or lengthening individual tension members which is equivalent to hypo- or hyper-to- nicity of the tensional network. (Refer to distortion images.) Using this model, it is possible to distort one or more tensile components (ligaments/muscles) and ob- serve the overall effect on the structure. (distortion image) Note that a change of length (or tension) in only one tensile component (e.g., the sacroiliac ligament or pelvic floor) causes distortions to oc- cur throughout the structure in all three axis’ (distortion images). In terms of this model a change in length of a tension component is equivalent to an increase or decrease in tension in that area. It could also be described more dynamically as a change in adaptation (i.e., the range of movement changes in response to a force acting upon it). Note that a change in a single tensile element is enough to cause the entire structure to be dynamically distorted. This model can also demonstrate gait and torsional movement, revealing the ten- sional net operating in the pelvis. As you articulate the struts, which represent the femurs, to simulate walking, you will no- tice the corresponding torque in the struts (x, y axis’) which are the ilia. By distort- ing a single tension element you can then observe the corresponding distortion in gait or rotation. Biomechanical function from a tensegrity perspective is a whole system explana- tion. Better description means better prescription, which means more success- ful treatment methods to benefit patients and clients.

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Page 1: quick ref singlepelvis1.6

A Biotensegrity Explanationfor Structural Dysfunctionin the Pelvis

In Biotensegrity modeling of the pelvis, the expanded octahedron tensegrity (as in the logo above) is a useful starting point. Because it is oriented along the fa-miliar ‘x, y, and z’ axis’ it is easy to sche-matize the pelvis which has equivalent orientations (left/right, top/bottom, front/back). Also this tensegrity has a central ‘cavity’ which expands or contracts and distorts, as forces are applied - a close analogy to the pelvic structure. This basic shape has been expanded to include the femurs and suggest the lower spine which is suspended and stabilized in the ten-sional network. The horizontal struts (x, and z axis’) illustrate the essential bal-ance of the ilia in relationship to the spine and femurs which are represented by the vertical (y axis) struts.

biotensegrity modeling

1.5 © 2005 intension designs ltd.

front view front view - distorted

side view - distorted

3/4 view - normal 3/4 view - distorted

top view

top view - distorted

side view

Single Tensioned Pelvismodel 05-STP-3.1

Pathomechanics of the pelvis and lower back can be illustrated by shortening or lengthening individual tension members which is equivalent to hypo- or hyper-to-nicity of the tensional network. (Refer to distortion images.) Using this model, it is possible to distort one or more tensile components (ligaments/muscles) and ob-serve the overall effect on the structure. (distortion image) Note that a change of length (or tension) in only one tensile component (e.g., the sacroiliac ligament

or pelvic fl oor) causes distortions to oc-cur throughout the structure in all three axis’ (distortion images). In terms of this model a change in length of a tension component is equivalent to an increase or decrease in tension in that area. It could also be described more dynamically as a change in adaptation (i.e., the range of movement changes in response to a force acting upon it). Note that a change in a single tensile element is enough to cause the entire structure to be dynamically distorted.

This model can also demonstrate gait and torsional movement, revealing the ten-sional net operating in the pelvis. As you articulate the struts, which represent the femurs, to simulate walking, you will no-tice the corresponding torque in the struts (x, y axis’) which are the ilia. By distort-ing a single tension element you can then observe the corresponding distortion in gait or rotation.

Biomechanical function from a tensegrity perspective is a whole system explana-tion. Better description means better prescription, which means more success-ful treatment methods to benefi t patients and clients.