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Chapter 5102Table 2. rTR and ATT during different movements in ACL-deficient, ACL-reconstructed and ACLintact knees.Kinematic variable ACL-deficient ACL-reconstructed ACL-intactRange of tibial rotation (in degrees; mean (SD))Level walking 13.7 (4.1) *(P=0.15,ns) 14.1 (3.9) †(P=0.12,ns) 17.3 (6.4)SLHD 16.9 (3.7) *(P=0.21,ns) 18.4 (3.4) †(P=0.64,ns) 19.4 (5.5)Side jump 16.6 (5.8) *(P=0.08,ns) 18.3 (4.7) †(P=0.24,ns) 20.7 (3.6)Anterior tibial translation (in mm; mean (SD))Level walking 4.6 (4.8) *(P=0.13,ns) 4.8 (5.4) †(P=0.25,ns) 6.6 (3.0)SLHD 9.3 (5.1) *(P=0.21,ns) 11.7 (9.2) †(P=0.60,ns) 13.4 (7.2)Side jump 6.7 (5.5) *(P=0.65,ns) 8.8 (7.5) †(P=0.78,ns) 7.7 (5.8)* paired t-test results comparing the ACL-deficient knee to the contralateral ACL-intact knee† paired t-test results comparing the ACL-reconstructed knee to the contralateral ACL-intact kneeACL = anterior cruciate ligament, SLHD = single-leg hop for distance, SD = standard deviation, mm = millimeter, ns = non-significant result. Figure 1. Example of results regarding the range of tibial rotation in both ACL injured knees (red lines) and ACL reconstructed knees (blue lines). The averages are depicted using the bold red and blue line respectively, The solid black lines represent the upper and lower limit of the range of rotation, in this example from the ACL injured knees.The Spearman’s correlation coefficients are displayed in Tables 3 and 4 respectively. Little (if any) to weak correlations were found between medial PTS, lateral PTS and Δ PTS and ATT for ACL-deficient or for ACL-reconstructed knees in all three dynamic tests. Little (if any) to weak correlations were found for ACL-deficient knees between medial PTS, lateral PTS, and ΔPTS and rTR in all three dynamic tests. In ACLreconstructed knees, these correlations were all moderate-to-strong, except for the correlations between lateral PTS and rTR during level walking and side jump (little (if any) correlation) and medial PTS and rTR during level walking (weak correlation).Mark Zee.indd 102 03-01-2024 08:56