Biomechanics of Hip Joint
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Transcript of Biomechanics of Hip Joint
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BIOMECHANICS OF HIP
Dr Siju K M
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Anatomy Ball and socket
synovial joint Head of the
femur articulateswith theacetabulum
Provides a high
degree ofSTABILITY &MOBILITY
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JOINT SURFACES HEAD : >1/2 of sphere Covered by hyaline articular cartilage
ACETABULUM : Lunate articularsurface covered by articular cartilagelatin : vinegar cup
SOURCIL :the area of bone above thesocket which bears the maximum load ofthe BW.. Entirely from the iliac bone
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STABILITY & MOBILITY Depth of acetabulum , narrowing of
mouth by acetabular labrum Tension & strength of ligaments Surrounding muscles Length and obliquity of neck of femur
MOBILITY DUE TO THE LONG NECKWHICH IS NARROWER THAN THEDIAMETER OF THE HEAD
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LIGAMENTS
FIBROUS CAPSULE ILIO FEMORAL LIGAMENT PUBOFEMORAL LIGAMENT ISCHIOFEMORAL LIGAMENT LIG OF HEAD OF FEMUR ACETABULAR LABRUM TRANSVERSE ACETABULAR
LIGAMENT
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CAPSULE PROX:acetabular labrum
including thetransverse acetabularlig
DIST :intertrochanteric line
anteriorly1 cm medial to
intertrochanteric crestposteriorlySynovial membrane
lines the capsule
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Iliofemoral lig (Bieglow) One of the strongest
ligaments of the body Prevents trunk from
falling backwards in
standing posture Inverted Y shaped APEX: lower part of
AIIS
BASE :Intertrochanteric lineas upper oblique andlower vertical bands
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Pubofemoral ligament Support
inferomedially Illiopubic
eminence,obturator crest&membrane toanteroinf part ofcapsule
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Ligament of head of femur
Flat &triangular Fovea capitis to
transverse acet lig &acetabular notch
Transmit arteries to
the head of thefemur
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Acetabular labrum Fibrocartilaginous rim
attached to themargins of the
acetabulum
Holds the head offemur in position
Narrows the mouth ofacetabulum
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Transverse ligament ofacetabulum
Part of theacetabular labrumwhich bridges theacetabular notchconverting it to aforamen which
transmits vesselsto the joint
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The neck of Femur Angulated in relation to the shaft in 2
planes : sagittal & coronal
Neck Shaft angle Anteversion
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Neck shaft angle Angle between the
neck and the shaftin sagittal plane
(viewed from thefront or back)
140 deg at birth 125-135 deg in
adult
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Anteversion Angle between the
neck and shaft inthe coronal plane
(viewed fromabove) Axis of the neck
and thetranscondylar axis
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Anteverted 40 deg at birth 20 deg in adults(15-25)
Ante version : ER of the head offemur in relation to the condyles
Retroversion : IR of the head of thefemur
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Acetabular Direction
Similar rotationaldifferences may alsobe found in theacetabulum
Usually long axis ofthe acetabulum pointsforwards :ANTEVERTED
The Acetabular axis ismore variable
ante version
retroversion
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Flexion 120 degree
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Extension 20 degree
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Abduction 50 degree
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Adduction 30 degree
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ER/IR 45 degree
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Chief muscle access ms
Flexion iliacus,psoas major pectenius,rectusfemoris,sartorius
Extension Gl maximus,hamstringsAdduction Add longus.magnus,brevis pectinius,gracilisAbduction Gl med,min TFL,sartoriusIR TFL,ant fibres of
gl med,min
ER 2 obturators,gamelli , piriformis,glmaximus,sartoriusquadratus femoris
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BIOMECHANICS
Center of mass The center of mass is the unique point at
the center of a distribution of mass inspace that has the property that theweighted position vectors relative to thispoint sum to zero.
Center of mass is the mean location of adistribution of mass in space .
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Center of gravity Center of gravity is the point in a body
around which the resultant torque due togravity forces vanish.
http://en.wikipedia.org/wiki/Resultant_forcehttp://en.wikipedia.org/wiki/Resultant_force -
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Subject standing on bothlegs
Little or nomuscular forcesreq to maintain
equilibrium
If support issymmetrical eachhip carries abt31% of the BW
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Trunk+UL 4/6 bwt LL 2/6
Each hip 1/3 Single leg stance 5/6
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Subject standing on one
leg Loaded hip supports the
mass of the head , trunk ,
UL and the other leg CoG lies farther awayfrom the loaded hip
Lever arm of BW is 3times the abductor leverarm
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Centre of gravity S5
BW vector K :(BW-Wt of loading leg)
runs thru S5 ..
medial to the non wtbearing hip
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Muscle balancevector M : Muscleforce to prevent
the left side of thepelvis from fallingdownward
Provided by theabductors actinglaterally to the hip
jt
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Compressive force R
Force acting on the hip Jt
Body Wt lever arm h
Muscular lever arm h
h=3h
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in equilibrium
Kh=Mh M=K (h/h)
Since h/h =3 M=3K
=3 times the body wt
Total force acting on theJoint R = K + M
= K+3K= 4K
4 times the body Wt
Total force acting on the joint when theSubject stands on one leg is almost
Equal to 4 times the body Wt
Coxa vara
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Coxa vara GT is higher than
normal Lenghtens the
abductor lever arm Changes the
direction of theforce M
Decrease in forceM Larger wt bearing
surface
Resultant force R is less thana normal hip
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Coxa valga GT is lower
Shortens theabductor lever arm
Changes thedirection of theforce M
Increase in force M
Resultant force R is more thana normal hip
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Biomechanics in limping PAIN MUSCLE WEAKNESS
Pelvis tilts to the AFFECTED side The body wt lever arm h is shorterin a limping patient.
The abductor lever arm is unaltered
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During the singlesupport phase ofgait the patientdisplaces the trunkto the affected sidebringing the CoGnearer the affected
joint whichrequires lessmuscle force to
balance the BW
Body wt K can be counterbalanced by a smallermuscular force and the resultant R is less
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Biomechanics in limping Limp is defined as any deviation from
the normal effortless gait Clinically we come across 3 types of
limp ANTALGIC SHORT LIMB TRENDELENBERG May be present as single or in
combination
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ANTALGIC GAIT DECREASED STANCE PHASE Bears wt on the affected side for as
short a period as possible Allows the load to remain the normal
hip for a longer time Attempts to protect the hip by tilting
towards the AFFECTED SIDE
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SHORT LIMB GAIT Equal amt of load bearing on either
side NORMAL STANCE PHASE Lurches towards the AFFECTED
SIDE
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TRENDELENBERG GAIT
NORMAL HIPDEPENDS ON
FULCRUM : hip jt LEVER : Neck of
femur
POWER : abductors
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TRENDELENBERG GAIT STANDING ON NORMAL
LEGThe CoG falls towards the
opp hip.The pt tries tomaintain the equilibriumby the power of theabductors which pull theorigin to their insertionthereby raising the opppelvis
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TRENDELENBERG GAIT STANDING ON
AFFECTED LIMB
Opposite pelvisDIPS DOWN due tothe abnormalabductormechanism of thewt bearing hip
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normal
affected
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TRENDELENBERG GAIT disorders causing the pelvis to sag onthe unsupported (opposite) side. This creates an uncompensated
Trendelenberg gait and a positiveTrendelenberg sign. If the upper body leans over the
affected (weak) hip, the pelvic sag iscompensated for and this is a so calledcompensated Trendelenberg gait orsign.
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Causes 1) Suprapelvic.
Costopelvic impingement as in scoliosis 2) Pelvic.
This is due to loss of the fulcrum asin developmental dysplasia of the hip; orof the lever mechanism as in nonunion ofthe femoral neck; or of power as inpoliomyelitis or muscular dystrophy.
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3) Infrapelvic. This is caused by medialdeviation of the mechanical axis of thelower limb .
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GAIT CAUSES STANCEPHASE
PELVICDIP
ANTALGIC Painanywherein the limb
DECREASED AFFECTEDSIDE
SHORTLIMB
Shorteningof anycause
NORMAL AFFECTEDSIDE
TRENDEL-ENBERG
Abn infulcrum ,lever,power
NORMAL NORMALSIDE
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Walking stick Use of a walking stick in the opposite
hand can reduce limping
It lessens the displacement of thetrunk to the affected side during thesingle support period
Exert force C on the stick with a lever arm f
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Exert force on the stick with a lever armForces C & K are vertical & opposite
The moment Cf tends toRotate the pelvis upwardWhile the moment Kh tends To rotate the pelvis down
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The resultant force F = K-C : F acts with a lever arm s which is
smaller than h The force K which normally rotates
the pelvis clockwise with a momentKh is replaced by F
Moment FS is smaller asF
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Stick and Limp Both decrease the moment of force
exerted by the body wt on theloaded hip
Stick :transmit part of the force tothe ground thereby decreasing themuscular force req for balancing
Limping shortens the lever arm byshifting the centre of gravity to theloaded hip
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p
Thank you