Determination of the Knee Joint Internal Loads During Deep Squat
by
CHRISTIAN E. SPANU
Abstract
The objective of the present work
is to determine the internal loads inside the knee joint during a deep squat
while the knee is maximally flexed, up to 150 degrees of knee flexion. A
two-dimensional anatomical mathematical model of the human knee joint was
developed for this purpose. To collect model input data, X-rays were first
obtained to determine the mathematical representation of the tibial and femoral
articular surfaces. An X-ray stand was specifically designed and built for this
purpose. An integrated human motion analysis system that includes two force
plates and a video camera based human motion measurement system was then
employed to measure ground reaction forces at different positions during deep
squat. The knee joint net equivalent loads - forces and moments – were then
determined using a stick diagram representation of the lower limb. This was
followed by the determination of the knee joint internal loads including
ligamentous forces, tibio-femoral contact force, and quadriceps and hamstrings
equilibrating forces. For this purpose, the knee joint has been modeled as two
rigid bodies, the tibia and the femur, undergoing general planar motion in the
sagittal plane. The tibia was assumed fixed while the femur slides and rolls
along the tibial plateau, without losing contact. Point contact was enforced in
the analysis. The model included ten ligamentous structures to represent the
cruciate and collateral ligaments along with the posterior capsule, and two
muscle forces: quadriceps and hamstrings. The quadriceps forces were applied
through the patellar tendon. Model calculations were conducted to simulate
isometric quad contractions associated with hamstrings co-contractions at
different positions during squat.
Results show that in deep flexion,
the femoral contact point occurs on the most proximal point of the posterior
condyle, and is located posteriorly on the tibia. The most anterior location of
the contact point on the tibia occurred when the subject was standing, and the
most posterior location occurred when the subject was squatting while the knee
was flexed. Increasing quad forces produced an increase in the tibio-femoral
contact force. Model calculations have shown that this contact force was much
larger at full extension than in flexion. Model calculations have also shown
that during the deep squat, hamstrings dominance was required to maintain
equilibrium at small flexion angles. As the flexion angle increased, equilibrium
was maintained with quadriceps dominance.
The posterior cruciate ligament
(PCL) was found to be the most important ligament in the squat. The anterior
cruciate ligament was found to carry loads only in a standing position. As the
flexion angle increased, the PCL and in particular its anterior fiber bundles,
were found to carry very high loads on the order of thousands of Newtons.
Numerical calculations have shown that at a given flexion angle, and as the
quadriceps force increases, the hamstring forces increase; and this was
associated with an increase in the PCL force.
This study represents a first
attempt to understand the knee behavior in weight bearing activities with
maximum knee flexion. These results clearly show the important role of the
posterior cruciate ligament in this position. This may be an important factor
when deciding whether to keep or remove this ligament when performing a total
knee replacement procedure. Furthermore, the present study shows that when the
knee is in deep flexion, contact occurs on the most proximal points of the
posterior condyles. This might explain why most commercially available total
knee replacements do not allow for maximum flexion angles: the proximal surface
of the posterior condyle is not resurfaced.
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