MODEL FOR STATIC LIFTING: RELATIONSHIP ON THE SPINE AND THE KNEE F. J. Division of Bioenginsering,
BEJJANI,
Hospital
C. M.
GROSS
and J. W.
for Joint Diseases. Orthopaedic
New York.
NY
OF LOADS
PUGH Institute.
301 East 17th Street.
lOW3. U.S.A.
Abstract-An experlmrntal study based on a trigonometric. anthropometric model. was conducted on thirty-five healthy subJccts 10 determine the relationship between knee and back forces during symmetric sagittal plane lifting. Total joint reaction forces for the knee and the back, along with their compressive and shear components, were calculated for each subject, as a function of the knee. back and ankle angles. The shear component was significantly higher in females than in males; the compressive component u’ab significantly higher in males. Strong inverse correlations were found between the back and the knee forces on all subjects. Strong correlations were also found between subject anthropometry and minimum and maximum joint reaction forces. The magnitudes of both back and knee joint reaction forces should be considered in recommending the lift type and position. based upon individual worker anthropometry. and Size and weight of the load-to be liftdd.
angle of flexion of the back . angle of flexion of the tup angle of Aexion of the knee angle between the foot and the leg angle between vertical and leg angle between Ihc thigh and the horizontal distance bctwcen acromion and third PIP joint. (ml distance bctwccn rl and the third coccygeal vertebra. <’ I
I II FE
FQ P
L, Lt.
LP I_;
2
L: L,, 11; II, % 111
CL3 SB JB CK SK JK
(m) distance between rl and vertex distance bcruecn greater rrochanter tip center of latcr;LI femoral condylc. (m) distance belwecn cenlcr oflutcral femoral condyla and heel. (m) height of the load. (m) erector spinac force, (N) quadriceps muscle force. IN) \reight of the load, (NI Icvcr arm of the arm about G, (m) lever arm of the erector spinae. (m) lever arm of the load about LCLS. (m) lever arm of the load about G, (m) lever arm of the quadriceps muscle, (m) leler arm of the head and torso about G, (m) lever arm of the rhigh about the center of rotation of the knee. G. (m) lever arm of It’1 about L4-LS. (m) uelght of the arms, (N) weight of the thighs. (NI uelght of the head and torso. (N) weight of the head, torso and arms (N) compression force on L-l-L% (N) shear force on L%LS. (XI total joint reaction force on L4-L.5, (N) compression force on the tibia-femoral joint, (N) shear force on the tibio-femoral joint. IN) lotal joint reaction force on the tibio-femoral joint, IN)
AJ
JB+ZJK 2 ISTRODC’CTION
The occurrence highest between
of low back pain in industry is the ages of 35 and 40 years (Calin er
al., 1980; Frymoyer rf rrl.. 1950). Knee joint arthritis usually appears later in life, with an age peak above 65. At this age, more than 2 ‘I(,of all men and 6.6 ‘I#,of all women in the United States suti-r from some degree of knee arthritis (U.S. Department of Health, 1971-75). Given that knee lifting is recommcndcd for back pain patients (Miller, 1980; Bendix and Eid. 1983: Swedish Back School), one would tend to think that ultimately there would be a greater incidence of knee arthritis among these patients. The purpose of the present study is to develop a model to predict loads at the knee as a function of relative participation of the back in lifting, and to evaluate the model using data taken from ths actual test subjects.
;\lODEL We used a simple. two-dimensional static model. based on trigonometry and anthropometry (Fig. I). The model represents the projection in a sagittal plane of the mechanical axes of the spine and the dominant upper and lower limbs of an individual. This position corresponds to the phase when weight is just about to leave the ground. The upper limb is vertical. The elbow is in full extension and slight pronation. The forearm is in contact with the patella. The proximal interphalangeal joints (PIP) are considered in contact with the handle. The foot is lying Rat on the ground. The angIes considered are the following (Fig. I):
ct = angle p = angle 0~- angle i i angle -angle of E = angle
of flexion of the back, of flexion of the hip. of Rexion of the knee. between the foot and the leg (= 90. dorsiflexion of the foot). between the thigh and the horizontal.
The anthropometric following (Fig. I): a = distance 281
measures
between acromion
considered
arc
the
and third PIP joint.
282
F. J.
BEJJANI. C. M. GROSS and J. W. PUGH
Fig I. Trigonometric and anthropometric model; IL = back Rexion angle; fi = hip flexion angle; y = knee flexion angle; E = angle between thigh and horizontal; 6 = angle between foot and leg; p = angle between vertical and leg; B = center of rotation of the hip; G = center of rotation of the knee; a = distance between acromion and 3rd PIP joint; b = distance between TI and 3rd coccygeal vertebra; c = distance between Tl and vertex: I = distance between greater trochanter and lateral femoral condyle; I = distance between lateral femoral condyle and heck It = height of the load.
between 7Y and third coccygeal vertebra, t = distance between greater trochanter tip and center of lateral femoral condyle, 1= distance between center of lateral femoral condyle and heel, c = distance between 7’l and vertex. h = distance
Considering the triangles CDL. QBG and WBQ (Fig. 1). we have the following trigonometric equation: lsinb+rsins+bcosa
= a+11
(1)
where h is the height of the load and the other variables are described above. A value for E can be obtained: & = 90’-(P-r). In the quadrilateral
ABGD
(9O+ca)+~+(180”-6)+(180’-‘J)=360”. Equations
(2)
(3)
(2) and (3) give us the following E = 180-y-6.
Equations (1) and (4) give us the following relationship coso! = (a+h)--Isin6-fsin(y+6) b
(4) angular
(5)
A free-body analysis was done on both the back and the knee (Frankel, 1980). For the back, we used the free-body above the L4-L5 joint, including the head, torso and arms (Fig. 2a). We obtained the erector spinae force, FE, by applying the moment balance
Ezb
Cb)
Ip
Fig. 2.(a) Free-body diagram above L4-L5: FE = erector spinae force; LE = lever arm of the erector spinae about L4-LS; VVJ= weight of the head, torso and arms; L, = lever arm of IV? about L4-LS; P = weight of the load; L, = lever arm of the load about L4-L5; JB = joint reaction force; C’B = compression force; SB = shear force. (b) Free-body diagram above the knee: N;. = weight of the head and torso; L, = lever arm of ‘.Vt,. about G (center of rotation of the knee); tVr = weight of the thigh; Lr = lever arm of W, about G: W’ = weight of the arm; FQ = quadriceps force; LQ = Lb = L, = lever arms of FQ, P,, and IV’ about G; JK = joint reaction force; CK = compression force; SK = shear force. equation
(all forces and weights are in Newtons) (WI x &.)+(P
x IL,)--(FE
x L,)
= 0
(6)
FEJ~xL,v)+(PxL,) L&
where 1%= WC (weight of head and torso)+ it> (weight of arms). According to Barter, W,. = 0.47 x total body weight + 54, WA= 0.13 x total body weight + 14, L,.= lever arm of WI about L4-LS, assumed to be = b/2sinz (Fig. Za), P = weight of load, L, = lever arm of load about L4-L5 assumed to be = absin z, L, = lever arm of erector spinae = 0.05 m. By projecting all the forces on two axes. one along the spine mechanical axis (compression axis) and one perpendicular to it (shear axis), and by applying the force balance equation, we then have (Fig. 2a) CB=
CMxcosz+FE
where CL? is the compression SE=
(7)
force on the back (L4- L5)
Wlxsina+Pxsinz
(8)
where SJ3 is the shear force on the back (L4-L5) JB = ,,‘CB’ f SB2
(9)
283
Mode! for static hftmg
H herr JB is the total Joint reaction force on the back (L4-L5). For the knee, we used the free-body above the knee. including the ipsilateral thigh and arm and half the sum of the head and torso. The moment equilibrium equation gives us the value of FQ. the quadriceps muscle force (Fig. 2b): I
FQ=jx
(-PxL,+lt;
xLc-w;+tt;x&l
LQ
-
(101
bt; and P have been defined above. itT = weight of the thighs = 0.18 x total body u-eipht + 15 (according to Barter, 1957) Lr = lever arm of the thigh about the center of rotation of the knee. G. Barter’s tables show the centerof-mass of the thigh at 56.7”,, of the thigh length (r) from G. The value of 4. is therefore: 4,. = 0.567 x I x cosE(Figs 1 and 2b); and if we solve for E in equation (4) L, = 0.567 x t x cos( 180 - y - 6), L, = (lever arm of the quadriceps muscle) = Lb = lever arm of the load, about G) = L,, (lever arm of the arm, about G) = 0.05 m. (approximate distance between the pat&r surface and G) (Fig. 2b). L, = lever arm of the head and torso, about G. Barter’s tables show the center-ofmass of the head and torso at 39.6”,, of h (defined above)+c (distance between 7l and the vertex). from the distal end of the spine. This and equation (41 give us:
where It;.
L, = I cos ( 1SO - ;’ - 3) - 0.396 (h + (‘1sinz (Figs 1 and 2b). By projecting all the forces mvolvcd on two axes. one along the thigh mechanical axis (compression axis)and one perpendicular to it (shear axis), and by applying the force equilibrium equation, we then have (Fig. 2b)
=!&
cK
+lt:,+&+P) 2
-sm(y+6)+FQ
(11)
where CK is the compression force on the knee (tibiofemoral joint). In equation (1 I), sin (y - b) = cos (;’ - 14) because /i = 90’ -d (Fig. I) sK
_
( 4 + Lb;+ y+ 2
PI
x (-cos(y+8))
(12)
where SK is thr shear force on the knee JK = ,‘CK=
-+sK2
(13)
where JK is the total joint reaction force on the knee*.
>lATERIALS
AZD
.\lETHODS
The anthropometric data were collected from 35 subjects, IS females and 17 males. Age range for the females was from 15.5 to 30, with a mean of I8 + 3.0.
* The patello-femoral joint reaction force bears a determinate relationship to geometry and extension force. and has not been addressed in this srudy.
Ape ranpr for the males was from 16 to ill. with a mean of 232 5. After recording Height and height. the subjects were positioned against a vertical gradicule for the folloaing measurements on the dominant side: distance between acromion and third PIP jotnt. distance between tip of the greater trochanter to the center of the lateral femoral condyls. distance between the center of the lateral femoral condyle to the floor. Then, using an anthropometric tape. the distance between Tl and the third coccygeal vertebra and between 71 and the vertex were measured. A computerprogram was urirten to solve the cquations previously derived. The knee angle (;) was allowed to vary from 0 to I20 by steps of 5 The ankle angle (6) was allowed to kary in 2 increments from 65 to 90 The back angle (z) was obtained from equation (5) and was allowed a maximum of 60 . because pelvic tilt would occur after that. The anthropometric measurements of each subject were entered and several sets of data were obtained. In the first set, weight and height of the load were constant for all the subjects: P = 5kg; h = 0.2 m. In the second set. height of the load was a constant (II = 0.2 m) and its weight took three diKerent values: lo”,,, 3X33”,,. and 50”,, of the total body weight of each subject. In the third set. weight of the load was a constant (P = 5 kg) and its height took three different values: IO”,,, 20”,, and 35”,, of the height of each subject. Each of these seven sets of data was tabulated for each subject under dlfrerent loading conditions. A *Table for Joint Forces’ (see Appendix) showed all the possible combinations of back. knee and ankle angles (60-80 combinations. dcpcnding on the subject) and corresponding values for all the forces involved. A new coefficient was added to help describe the global forces on the body:
JB + ZJK AJ = p-. 2 The program wasalso set to pick minimal and maximal values for each of these variables and print them separately with the corresponding combination ot’ angles and forces. All data collected were analyzed statistically, using the SPSS package (Version 8). Two major studies were performed: a comparison between back and knee forces for each subject and a comparison between males and females.
RESULTS AhD
DISCLSSIOS
A very high inverse correlation was found between knee and back forces for all subjects (Table I). The graph of knee joint reaction force as a function of lumbar spine joint reaction force displays an inverse quasi-linear relationship (Fig. 3). As the knee takes an increased amount of load. spinal load is decreased. Another strong correlation was found between the anthropometric measurements and the minimal and
284
C. M. GROSS and J. W.
F. J. BUJANI.
PLGH
Table I. Pearson Correlation Table between the forces on the back and the knee for subject no. 32: age = 28; sex = M; dominant = R; weight = 83 kg; height = 1.68 m; b = 0.54 m: a = 0.69 m: t = 0.38m; I = 0.5 m; c = 0.26 m Total joint reaction
Knee Back
Shear
Compression
Shear
0.866 p < 0.001 0.864 p
- 0.980 p
Compression Total joint reaction
maximal
values
anthropometry
of
JK
JB.
and
was summarized
AJ
- 0.987 p
p
(Table
2). The 903
in three major com-
I 3000 Back jomt reaction
25CO
ponents for this purpose: distance between the vertex
fwce
.
I 3500 IN
1
and the distal end of the spine, upper limb Length, and lower limb length. This correlation and corroborates
was accounted for
the work of Tichauer
(1968), Mital
PI al. (1980), and others in the prediction capability,
of lifting
Fig. 3. Graph of the knee joint reaction force as a function of the back reaction force (p < 0.001) for subject no. 32 (see Table I). when lifting position isallowed to vary. This pattern was consistent among al! subjects.
based on somatotype.
In order to compare
males and females. the mean
There
was also a significant
pression
dividing
to
Females appear to respond more in shear and males in
minimize factor.
total
the role of the individual
The
test (Table
ratios were compared 3). There
body
was a significant
ratios
being greater
difference
ratios
greater
for
the
be-
The coefficient AJ = (JB + 2JK)/2
back and knee for females.
an acceptable body. Under
representation the different
was considered
of average force on the
load conditions
above. this coefficient was computed
mentioned
for each subject
Table 2. Pearson Correlation Table for all subjects, between the anthropometric measurements and the minimal and maximal values for the joint reaction forces on the back and the knee, and the coefficient AJ = (JB + 2JK)/2 JB minimum
Forces anthropometry Vertex to coccyx Acromion to 3rd PIP joint Great trochanter to floor
JB
JK
JK
AJ
AJ
maximum
minimum
maximum
minimum
maximum
0.92
0.89
p < 0.005
p < 0.005
0.57
0.54
p < 0.005
0.65
0.71
p < 0.005
p < 0.005
0.47
p < 0.005
0.76
p < 0.005
0.83
p < 0.05
0.62
p < 0.005
0.53
p < 0.005
0.15
p < 0.005
0.72 p < 0.005
0.34 NS
p < 0.005 0.75
p < 0.005
Table 3. Student’s t-test table between male and female subjects for the ratios of the mean forces over the body weight (Ii’) Mean force/ Body weight
Sex
N
Mean
S.D.
SB,W
F M
17 16
SKJW
F M
17 16
CB/W
F M
CK/W
F M F M
17 16 17 16 17 16
F M F M
17 16 17 16
0.62 0.59 0.19 0.17 3.8 4.07 1.66 1.58 3.85 4.11 I .68 1.60 6.83 6.94
0.041 0.033 0.017 0.005 0.39 0.451 0.187 0.202 0.389 0.449 0.185 0.202 0.585 0.421
JB/W JKjW AJjW
males.
compression.
anthropomorphic
with a Student’s I-
tween males and females for normalized
shear forces, with
weight
with
in back com-
by
it by the subject’s
force
difference
was taken for each one of the forces and normalized
f
P
2.356
< 0.05
4.642
< 0.005
- 1.834 1.178 - 1.773 1.184 -0.623
< 0.05 NS < 0.05 NS NS
0.18 p < 0.005 0.78 p < 0.005 0.73 p < 0.005
285
Model for static hfting
and
the set of angles
responding
to optimal
These optimal weight
(knee.
back
(minimal)
angles were plotted
(Fig. 4) and as a function
and .&I
optimization
in either
was IO”,, of body flexion
(56
minimize
weight.
cor-
as a function
of load
of load height (Fig. 5).
The ankle angle did not significantly force
ankle)
was retained.
influence
case. When
optimize similar
33 “,,_ both
,-I./. At
angles
total force on the body varies significantly
as a function
of
load weight
characteristics,
and does not follow
) and the back. in extreme tlenion 159‘) to
bending Bejjani.
the anthropometry
and
an optimal
the knees to save the back’
(Miller.
1983).
(I 10
for the knee and 76 for the back). When height of the
This study is staticand
load was IO”,, of body
height
to shed light on the interrelatedness
moderately
and the back extremely
bent
(59‘) to optimize
(91’)
(Fig. 5). the knees were bent
AJ. At 20”,,. the back angle stayed the
the knee angle
decreased
significantly
to
quantitative:
of the knees and the spine during particular.
that for lifting
representing
its main purpose between
lifting.
minimize Forces’
We shovved. in
IO”,, of total body weight, one must bend
A-
) in order to
I 33 33
Body
weqht
I 50 I%)
Fig. 4. Graph of the optimal back knee and ankle angles as a function of the weight of the load (estimated in “,, body height). for a constant height of the load. Mean and standard deviation for all subjects. are considered for each joint angle.
I x7
IG i3oay
be produced
demands
Knee Bock
I
should
a ‘Table
as an aid
for Joint
in reducing
on the musculoskeletal
system.
A(.~nowl~d!/cmmrs-Mr. Keith losephson for his tine programming. Ms. Rirgitta Nilsson and \fr. Gillcs Demculenacrc for thctr excellent graphic work. Jnd to Ms. Toby Z. Licdcrman for her careful editing and t!p)ng
-‘\‘-IO
the average force. Ideally.
cumulative
is
function
a load of 0.2 m hetght and
both back (about 60 )and knees (about 90
0
of
1980;
.4J. At 50”,,.
the angles did not change much for either joint
:
the load
the princtple
PI./. At 33.33 l’l). the knees had to bend more
and the back less to maintain
same and
m a
This last phase of the study shows that the best way to minimize
average
the knee was in moderate
decreased
manner.
height
I 35 I%1
Fig. 5. Graph of the optimal back. knee and ankle angles as a function of the height of the load (estimated in ‘I0 body height). for a constant weight of the load. Mean and standard deviation for all subjects. are considered for each joint angle.
Bandi. W. (1972) Chondromalcia patellae and femoropatellarc arthrosc. H&. c&r. rlcrcl 1. 3. Barter. J. T. (1957) Estimation of Mass of Body Segments WADC Technical Reports: 57--X0. Wright- PJttrrson. OH. Bejjani. F. J.. Gross. C. M. and Pugh J. W. (1953) Stress relationship bctucrn the knee and the back. Proi &itt,s (d rl)c, Inrcnwriotrtrl Swicr~~jiw //IL, f_un~hcr Spiw. CJmbridgc. U.K. Bendix. T. and Eid, S. E. (1983) The distance bctaeen the load and the body with three bi-manual lifting techniques. rlppl. Eryonomics 14, 185. 192. Calin, A., Kaye, B.. Stcrnbcrg. M., Antcll. B. and Chart. M. (1980) The prevalence and nature of back pd)n rn and industrial complex. Spine 5, ZOI--205. Garg. A.. Mital. A. and Asfour, S. S. (19SO) A comparison 01 tsometric strength and dynamic lifting cdpabtlity. Er~o”o”tics 23, I! --27. Frankel. V. H. and Nordtn. M. (I 980) Blrstc Bionw, hrrics q/ r/w SLA~IU/ S.nrrm. p. 255. Lea & Febigcr. Phli~delphia. Frymoyer, J. W., Pope. M. H. and Costanza, hf. C. (1980) Epidemiologic studies of low-back pain. Spiw 5, 419423. Hungerford, D. S. and Barry, M. (1979~ Biomcchanrcs of the patellofemoral joint. C/in. Orrhop. Rd Rcs. 111. 9-15. Matthews. L. S., Sonstegard. D. S. and Henke. J. A. (1977). Load bearing characteristics of the patello-fernor Joint. Acclr orrhop. SC~~I!l
286
F. J. BEJJAX C. M. GROSS and J. W. PUGH
APPE\DIS.
TABLE FOR JOINT FORCES
Subject: JR. Age = 28 years. 5 months. Sex = male. Dominant side = right. Height = 1.68 m. Wetght = 93 kg. Somatotype factor = 0.0625162. Distance between rl and third coccygeal vert’bra = 54 cm. Distance between rl and top of head = 26 cm. Distance between third coccygeal vertebra and top of head = SO cm. Distance between acromion and third PIP joint = 69 cm. Distance between greater trochanter and femoral condyle = 38 cm. Distance between heel and lateral remora1 condyle = 48 cm. Distance between greater trochanter and heel = 86 cm. Box height = 20cm.
x”
i.0
60
FE (N)
FE/W
59 5s 57 56 56
85 85 85 S5 90
69 71 73 75 65
3259 3233 3202 3167 3176
4.00 3.97 3.93 3.89 3.90
56 55 54 53 52
90 90 90 90 90
67 69 71 73 75
3152 3123 3090 3052 3010
52 52 51 50 49
95 95 95 95 95
65 67 69 71 73
48 48 47 46 45
95 100 100 100 loo
44 43 43 42 41
FQ (N)
Box weight = 10 kg
FQjM’
SE (N)
SK (N)
CB (N)
503 542 5SI 619 54s
0.61 0.66 0.71 0.76 0.67
561 556 551 545 547
365 371 377 382 368
3592 3573 3551 3525 3532
681 70s 733 755 720
3636 3616 3593 3567 3574
773 799 a24 819 sG9
3.87 3.S4 3.79 3.75 3.70
556 622 65S 693 728
0.72 0.76 0.8 O.S5 0.89
542 538 532 525 51s
374 379 3S-l 389 393
3514 3492 3439 3406
745 769 791 812 834
3555 3534 350s 3479 3445
a34 857 579 901 922
3026 2995 2959 2919 ‘873
3.72 3.6S 3.63 3.58 3.53
670 704 737 770 802
0.82 0.86 0.9 0.94 0.98
521 515 509 502 495
382 386 391 349 398
341s 3395 3367 3335 3299
809 830 849 868 887
345s 3434 3405 3373 3336
595 915 935 954 972
75 65 67 69 71
282 I 2845 2807 2764 2714
3.46 3.49 3.45 3.39 3.33
834 7SS 819 849 879
I .02 0.96 1.00 1.04 1.OS
486 490 483 476 467
400 393 396 399 401
3257 3276 3245 3210 3170
905 894 910 927 943
3293 3312 3281 3245 3204
990 976 993 109 103
100 loo 105 105 IO5
73 75 65 67 69
2659 2596 2628 25s I 252S
3.26 3.19 3.23 3. I7 3.10
909 939 905 933 961
1.1 I 1.15 1.1 I 1.14 I.18
458 447 452 444 435
403 405 400 402 404
3124 3072 3098 3059 3014
959 975 976 989 1003
3157 3104 3131 3091 3@46
IMO 1056 1055 106S iOS7
40 39 37 38 37
105 105 105 110 110
71 73 75 65 67
2468 2401 2325 2365 230S
3.03 2.95 2.85 2.90 2.83
988 1017 1046 1023 1049
1.21 1.25
425 413 400 407 397
405 406 406 405 406
2964 2906 2840 2875 2825
LO17 1031 1046 1059 1070
2994 2935 2868 2904 2553
1095 IIOS 1122 1134 1115
36 34 33 31
110 110 110 110
69 71 73 75
2242 2169 2085 1990
2.75 2.66 2.56 2.44
1075 1102 1130 1160
1.32 1.35 1.38
386 373 359 342
406 406 406 405
2768 2704 2630 2546
1082 1095 1109 II24
2795 2729 2654 2569
II56 1168 IlSI 1195
I.28 1.25 1.29
1.42
CK (NI
JB (N)
JK IN)