| Literature DB >> 35782284 |
Roman Trobec1, Gregor Kosec1, Matjaž Veselko2.
Abstract
Broadly accepted is that most knee injuries result from increased vertical forces, usually induced by an incidental ski fall, collision, or a high jump. We present a new non-contact knee injury mechanism that can happen during a ski turn. Such an injury is governed by a sudden inward turn of the inner ski and consequent swing of the inner leg followed by a nearly instant stop when locked by hip and knee joints. The model provides predictive results for a lateral tibial plateau compression fracture because several simplifications have been made. We confirmed that the modelled compression stresses at typical skiing conditions and with typical skiing equipment can provoke serious knee injuries. The awareness of skiers and skiing equipment industry of the described knee injury mechanism can act as an important injury-prevention factor.Entities:
Keywords: Biomechanical model; Compression fracture; Knee; Lateral tibial plateau; Non-contact injury
Year: 2020 PMID: 35782284 PMCID: PMC9219317 DOI: 10.1016/j.smhs.2020.08.003
Source DB: PubMed Journal: Sports Med Health Sci ISSN: 2666-3376
Fig. 1Coronal (a), sagittal (b) and transverse (c) images of the right knee of patient with a lateral tibial compression fracture that occurred during a right carved ski turn, i.e. right inner ski. Image (a) was used for a determination of leg rotation constraints.
Fig. 2The scheme of accident (illustration drawn by J. Polajnar) with the following abbreviations for model variables:
m1 – mass of skier's upper part of body with an outer leg, ski and ski boot,
m2 – total mass of inner leg with ski and ski boot,
m21 – mass of upper part (femur) of inner leg,
m22 – mass of lower part (tibia) of inner leg,
m23 – mass of ski and ski boot,
L – inner leg length,
v0 – skiing velocity,
ω – angular velocity,
ΦC – final value of inner leg angle,
β – angle between femoral and tibial axes after a fracture,
ε – centre of rotation in the inner leg knee joint,
A – estimated area of depressed tibial plateau.
Fig. 3Four video frames taken from a video sequence of a real incident recorded by coincidence.
Set-up of the validated case with the following abbreviations for model variables and units:
m1 – mass of skier's upper part of body with an outer leg, ski and ski boot,
m2 – total mass of inner leg with ski and ski boot,
m21 – mass of upper part (femur) of inner leg,
m22 – mass of lower part (tibia) of inner leg,
m23 – mass of ski and ski boot,
L – inner leg length,
ε – centre of rotation in the inner leg knee joint,
A – estimated area of depressed tibial plateau,
β – angle between femoral and tibial axes after a fracture,
v0 – skiing velocity,
kg – kilogram,
m – meter,
m2 – square meter,
rad – radian (angle),
m/s – meter per second (velocity).
| 90 | 16.5 | 6.0 | 4.5 | 6.0 | 1 | 0.03 | 3.7 × 10−4 | 0.52 | 15 |
Fig. 4Pressure on the lateral tibial plateau (P) as a function of the skiing velocity (v0) and the mass of ski and ski boot (m23). The red dot is the pressure P = 177 MPa obtained with data from Table 1. The red line marks the ultimate compressive stress 143 MPa that can be exceeded at v0 higher than 13 m/s and can cause a compression fracture of the tibial plateau. SI units: kg – kilogram, MPa – megapascal, m/s – meter per second.