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HISTORICAL RESEARCH REPORTResearch Report TM/85/01
1985
Manual handling: limits to lifting Graveling RA
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Manual handling: limits to lifting
Graveling RA This document is a facsimile of an original copy of the report, which has been scanned as an image, with searchable text. Because the quality of this scanned image is determined by the clarity of the original text pages, there may be variations in the overall appearance of pages within the report. The scanning of this and the other historical reports in the Research Reports series was funded by a grant from the Wellcome Trust. The IOM’s research reports are freely available for download as PDF files from our web site: http://www.iom-world.org/research/libraryentry.php
HISTORICAL RESEARCH REPORTResearch Report TM/85/01
1985
ii Research Report TM/85/01
TM/85/1UDC: 612.76
MANUAL HANDLING : LIMITSTO LIFTING
R A Graveling
January 1985
Price: £10.00
MANUAL HANDLING : LIMITS TO LIFTING
Contents Page No
1. INTRODUCTION 1
2. ASSESSMENT OF CRITERIA 3
2.1 Biomechanical Criteria 3
2.1.1 Intradiscal Pressure 32.1.2 Intra-Abdominal Pressure 72.1.3 Electromyography and Muscle Strength 14
2.2 Psychophysical Criteria 182.3 Metabolic Criteria 22
3. A 'HYBRID1 CRITERION 25
4. HEALTH AND SAFETY COMMISSION: REGULATIONS AND GUIDANCE 28
5. CONCLUSIONS 28
6. REFERENCES 30
ERG2/3
MANUAL HANDLING ; LIMITS TO LIFTING
R A Graveling
1. INTRODUCTION
Published limits can be divided into three broad categories*
Acceptable limits, derived from studies of what a worker is willing to lift
or carry. Safe limits, based on some physiological or biomechanical
criterion level which it is considered potentially harmful to exceed and
Official or Legal limits. These latter limits might be expected to reflect
those set according to the previous two categories. However, they may
sometimes be based on political expediency. For example, Carter (1969)
commented on the frequency with which 50 Kg or 1 cwt, commonly occurring
package weights, have been cited as limits in the national standards of
various countries. It could however be argued that the use of these weights
has evolved over years of experience and has some intrinsic validity as an
acceptable load.
The establishment of limits is complicated by the diversity of factors
which have been reported as influencing the amount which an individual can
lift or carry. Drury and Pfeil (1975) listed over twenty variables which
could affect lifting or carrying performance, classified under three general
headings of 'operator variables', 'task variables' and 'environmental
variables'. This list, adapted to Table 1, is by no means exhaustive, but
does give an indication of the complexity of the problem.
Table 1 Variables Potentially Affecting Lifting Performance(based on Drury and Pfeil, 1975)
Type Variables
OperatorVariables
SexAgeSizeStrengthSkillMotivationMethod of lifting
Task Variables Size of object liftedShape of object liftedPosition of handlesHeight at start of liftHeight at end of liftTime for which object is supportedDistance over which object is carriedFrequency of lift
EnvironmentalVariables
Temperature/humidity/air movementLighting, noise, chemical environmentSize and layout of workplaceDiscrete hazards (stairs, corners,slippery floors etc)
Various criteria have been adopted in determining what constitutes a
safe or acceptable lifting limit. Garg and Ayoub (1980) classified these
under three categories: (1) biomechanical: used to determine safe lifting
limits, (2) psychophysical: the determination of what is acceptable to a
person required to lift, and (3) metabolic/heart rate. This third category
reflects the physiological parameters usually adopted in establishing
criterion levels and is used to assess repeated lifting demands over a
period of time. Such parameters are not appropriate for the assessment of
single lifts.
2. ASSESSMENT OF CRITERIA
2.1 Biomechanical Criteria
2.1.1 Intradiscal pressure
One of the most widely adopted biomechanical criteria is that of the
compressive force acting on the vertebral discs. Such forces can be
directly related to those necessary to damage discs. Studies on'discs
obtained from cadavers showed a mean 'yield pressure1 of 710 Ibs (321 kg)
with a range of 350-1400 Ibs (158-634 kg) (Bartelink, 1957). These
pressures should probably be regarded as lower limits as the discs examined
were mainly from people of 60-80 years of age. A value for a younger person
has been quoted as 600 kg (Nachemson, 1966). Measures taken in vivo with a
needle inserted into the disc showed that, in a subject holding a 10 kg
weight in each hand and bending forwards at an angle of 20°, total
intradlscal pressures of between 250 and 340 kg could be recorded
(Nachemson, 1965). Resting values with the subjects standing in a relaxed
posture were 80 - 140 kg total load (588 - 883 kPa). More recently, resting
values of 331 ± 34 kPa have been quoted (Andersson et al, 1977). Although
the actual values are considerably different, possibly a function of
improved measurement techniques, again they found an increase in pressure
proportional to the back angle, with the pressure linearly related to the
sine of the angle. Similarly, for a fixed back angle, a linear relationship
was demonstrated between load and spinal pressure.
Fish (1978) described the calculation of the compressive forces
associated with lifting a 20 kg load by two different methods (straight
back/bent knee and flexed back/straight knee) and repeating the flexed back
lift with a 0.2 kg load. Forces were calculated for the L4/5 disc. The
mean values obtained (351 kg and 383 kg for 25° and 40° back angles) are
remarkably similar to those measured directly by Andersson et al (1978)
again for a 20 kg load (326 kg at 30°) despite apparently not allowing for
the support provided by the abdominal musculature (see below).
The degree of agreement between predicted and measured spinal forces
were reported by Schultz et al (1982). Studies were carried out with a
variety of arm positions and weights in sitting and standing postures. The
regression analysis of predicted compression forces against intradiscal
'pressure yielded a straight line with a correlation coefficient of 0.98.
Although the actual regression equation was not cited it can be seen from
the graphical presentation of the data that the origin is quite close to
zero on both axes but that the predicted force is consistently greater than
the measured pressure (slope > 1). The authors also cited earlier work by
Nachemson (1960) reporting in vitro studies which showed a direct
relationship between the compressive force actually applied, and disc
pressure.
The studies by Andersson et al and Fish showed a similar pattern of
results with an increase in disc compressive forces with increased load.
Neither study however showed any significant differences between the forces
associated with the two lifting methods. Andersson et al (1978) reported
that all means of peak force values were higher in back lifting whereas the
figures published by Fish (1978) showed the early stages of leg lifting to
result in;higher calculated forces than back lifting.
Ayoub and El-Bassoussi (1978) also published calculated spinal forces
(L4/5) for back and leg lifting of different weights, again showing a linear
increase in calculated force with increased load* They reported that
maximum compressive forces for back lifting were clearly higher than those
for leg lifting although no level of statistical significance was reported
and one figure, showing the time course of changes during a lift, showed
remarkably similar initial curves for both lifts with an unexplained
secondary maximum for the leg lift.
Unlike Fish (1978), Ayoub and El-Bassoussi do reportedly allow for the
effect of abdominal pressure in their calculations. However, despite this
fundamental difference, the compressive forces at the start of the lifting
cycle are very similar when the differences in load lifted are allowed for.
Thus, interpolating between values of 433 kg for a. 20 kg load and 246 kg for
a 0.2 kg load (Fish, 1978) gives a prediction of 287 kg for a 4.53 kg load
compared with the value of 280 kg (from graphical display) calculated by
Ayoub and El-Bassoussi.
The calculations of Fish differ in one major aspect from those of Ayoub
and El-Bassoussi or the direct measurements of Andersson et al. The former
paper does not indicate any real increase in compressive force after the
onset of a lift (two graphs showing an increase of the order of 5%, one a
decrease of a similar magnitude). However, the latter papers both show a
considerable increase. Ayoub and El-Bassoussi calculate an initial increase
of 37-47% Whereas the graphs reported by Andersson et al suggest changes of
the order of 100%.
Apart from a rather rudimentary comparison of two simple lifts, neither
of the two papers dealing with calculated spinal forces has any real
discussion of the application of their work. Neither paper commented on the
fact that, even with comparatively low loads, the calculated forces were
greater than those which, as detailed above, can destroy a disc. Similarly,
no attempt was made to apply this or any other criterion to determine
lifting limits. The calculations were, in both cases, limited to examining
the effects of increased load and to comparing the time course of force
changes during two 'idealised' lifts.
A recent NIOSH report on manual lifting (NIOSH, 1981) utilised data
published by a number of authors based on a variety of techniques including
disc pressure to develop criteria and subsequent lifting limits. The report
concluded that:- ' jobs which place more than 650 kg compressive
force on the low-back are hazardous to all but the healthiest of workers.
In terms of a specification for design a much lower level of 350 kg or lower
should be viewed as an upper limit'. Working on a mixed population, the
report uses data for an average female to produce the lower (350 kg) limit
and an average male for the upper (650 kg) limit.
Calculations based on a static loading model resulted in lower limiting
values of 4.5-83 kg and upper limits of 22-100 kg depending on the
horizontal and vertical location of the load, and assuming the 'best*
posture in each case. However, calculations for an average male, based on a
dynamic lifting model, indicated that 400 kg compressive force would be
generated by loads as light as 2-8 kg for leg lifts and 2-4.5 kg for back
lifts, varying according to horizontal location. Interpolating between the
600 and 700 kg lines gives 650 kg values of 16-55 kg and 13-45 kg for leg
arid back lifts respectively.
Despite these conflicts, the report nevertheless concluded that back
compressive forces could be used to produce practical recommendations for
acceptable lifting tasks and, subsequently, used spinal force criteria in
conjunction with others to produce composite lifting limits (see-below).
However, a more recent publication (Hutton and Adams, 1982) reported
substantially higher compressive strengths for spinal discs. The authors
hypothesised, that whereas in previous studies compressive forces had been
applied perpendicularly, with the two faces of the intervertebral disc
parallel, discs were flexed in vivo, and that this may alter their
compressive strength. Consequently, they examined compressive strengths of
discs over the probable range of flexion angle and consequent shear
component encountered in life. A sample of 16 disc specimens from 8 male
cadavers aged 22-46 years yielded a mean compressive strength of 10, 219 N
(sd ±";1711N), considerably higher than the figure of 6376N (650 kg) cited by
NIOSH (1981) as 'hazardous to all but the healthiest of workers'.
In an illustration of the significance of this finding, the authors
calculated that an average young male would need to increase his maximum
lifting strength by 44% before he could lift enough to crush his average
strength lumbar disc, assuming that no relief was provided by the intra
abdominal pressure (see below). No publication has been found to date which
modifies the biomechanical criteria to accommodate these revised data.
Direct measurement of disc pressure during load holding or lifting has
been carried out, but only in a clinical environment. Andersson et al
(1978), carried out direct measurements of the disc pressure during
laboratory lifting simulations, but concluded that such measurements were
not possible in field studies. It therefore appears from the literature
that, despite its intrinsic validity as a measure of lifting strain,
intradiscal pressure is not a feasible measure outside the clinical
laboratory.
Several groups of workers have calculated disc forces through
biomechanical models and, as cited above, Schultz et al (1982) have
demonstrated a close agreement between predicted forces and measured
pressures in the disc. However, apart from the NIOSH document, these
predictive models have not been used to produce any limiting lifting
criteria. In addition to the conflicts between the models, such as these
described above, most predictive programs published to date are based on
symmetrical, two-handed lifts in the sagittal plane (ie, the 'simplest1
possible lift). Frequently, the model is essentially static, generating
'movement* through a series of static postures rather than a genuinely
dynamic model incorporating inertial forces etc. They are therefore of
limited utility for industrial application.
2.1.2 Intra-Abdominal (intragastric) pressure
Another parameter examined by Andersson et al (1978) was the pressure
in the abdominal cavity, the intra-abdominal pressure or, more correctly,
as it is actually measured within the stomach, intragastric pressure.
Bartelink (1957) examined the intra-abdominal pressure using a stomach
balloon attached to a mercury manometer, in order to attempt to find a
possible explanation for the discrepancy between the measured forces for
destroying spinal discs of 158-634 kg, referred to earlier, and theoretical
predictions of the load placed on the base of the spine on lifting a 100 Ib
(45.4 kg) weight of 1600 Ibs (726 kg). It was found that when the back was
bent so that the hands were placed on the floor (or as near to the floor as
possible) the intra-abdominal pressure was comparatively low. As the trunk
was raised, the pressure rose to a maximum, the exact position of which
appeared to depend on the load being lifted but which occurred at about the
'half-way' stage. The pressure then dropped to a minimum with the subject
standing erect. As with the intradiscal pressure, the intra-abdominal
pressure was greater with heavier loads. Bartelink hypothesised that the
'abdominal balloon' as he described the abdominal cavity, and the muscles of
the trunk, in particular the transverse abdominal muscles, acted to provide
a 'muscle skeleton' which transmitted some of the load to the pelvic girdle
thus reducing the forces acting on the spine.
Eie et al (1962) reached the same conclusion as a result of their
"'studies on weightlifters. With more sophisticated equipment they were able
, .to study the pattern of changes far more closely than the earlier work with
_ a mercury manometer. Intra-abdominal pressure, again measured with a
stomach balloon was found to rise with forward bending of the trunk,
reaching a maximum when the trunk was at an angle of approximately 45°.
Higher pressures were reached during lifting than during lowering. As with
the previous study, pressures were found to be proportional to the weight
lifted. One item of particular interest was the markedly higher pressures
reached when a load (10 kg) was lifted incorrectly. Correct lifting
produced a pressure rise of 8-10 mm Hg whereas the abdominal pressure rose
by 50-60 mm Hg if the load was raised or lowered incorrectly. It was
concluded that the raised intra-abdominal pressure tended to counteract the
compression of the lower vertebrae and discs and made it possible for loads
to be lifted which would otherwise cause spinal damage.
In a recent review, Andersson (1980), referred to this hypothesis
stating that, although the positive relationship which had been demonstrated
between intra-abdominal pressure and biomechanical force analyses supported
the idea, further studies were necessary to test the hypothesis. Troup
(1979), however, described the mechanism for this supportive role,
suggesting that the abdominal musculature could take as much as 25% of the
overall compressive force induced by a load, particularly when the trunk was
flexed.
Andersson et al (1978) reported a series of experiments which examined
the effects of posture, and static (pulling) and dynamic (lifting) loads, on
the intradiscal and intra-abdominal pressures and the electromyographic
signals from back muscles. It was found that all three variables responded
systematically to changes in posture and load.
Davis et al (1964) examined intra-abdominal pressure (intra-gastric
pressures) and intrathoracic pressures during pushing, pulling and lifting.
It was found that the pressure changes displayed two clear phases. These
were an initial sharp increase, the 'snatch* pressure followed by a
sustained but lower pressure while maintaining the load. This pressure was
sometimes no greater than the resting pressure. Pressures in the thoracic
cavity (measured by a balloon in the oesophagus) were generally lower than
those in the abdomen. As would be expected, higher snatch pressures were
observed in those subjects who tended to jerk in the initial stages of the
movement whereas those who adopted a slower, smoother, approach generally
produced lower pressure changes. Intra-abdominal pressure changes, either
snatch or sustained, most commonly occurred and were of a greater magnitude
in pushing, with lifting second and pulling last. They were again found to
be related to the weight moved. It was concluded that pulling was the least
likely to overstress the trunk and that it was preferable to carry out the
manoeuvre in a slow, smooth fashion without jerking.
The measurement of intra-abdominal pressure was applied to a simulated
'real' task by Davis et al (1966). Three different procedures were studied
for raising one end of pit props in restricted headroom. Intra-abdominal
pressure measurements was carried out with radio pills rather than gastric
balloons, a useful development which allowed the subjects more freedom of
movement and presumably produced less discomfort. The pressure changes were
again studied in two ways, the peak pressure and the pressure-time product
(FTP), a development of the sustained pressure studied earlier by the same
authors. One lifting procedure produced significantly lower values for both
parameters than the other two. Again, speed of lift was shown to be an
important factor in determining peak pressure. However, when PTP was
plotted against speed of lift (lift time) it was found that the lowest PTP
values occurred at a time approximately one third as long again as the
fastest lift. It was suggested that this might be a valuable measure for
determining optimum rates for a particular manoeuvre. One matter for
caution referred to by the authors was that, although one particular lift
produced the least strain as shown by the pressure measurements, the body
movements resulted in an unstable working position towards the end of the
maneouvre. Clearly therefore, in assessing work routines, pressure
measurements should not be' considered in isolation, but in conjunction with
other parameters.
Davis and Stubbs (1977a) developed loading criteria based on intra-
abdominal pressure (IAP). They reported previous work in the construction
industry (Stubbs, 1973) which had shown an increased liability to back
injury in those members of the workforce carrying out tasks known to produce
frequent peak IAF values above 100 mm Hg. Adopting a 10% safety margin
(Davis and Stubbs, 1978b) they subsequently carried out an extensive series
of laboratory studies to determine the external forces exerted by lifting,
pushing and pulling in various postures which would induce IAP values of
90 mm Hg. These values were first published for small (5th percentile)
males, under 35 years of age (Davis and Stubbs, 1977a, 1977b and 1978a).
They were subsequently republished with additional data for different age
groups (Materials Handling Research Unit, 1980).
One slight anomaly in the figures presented is that the force data are
those for workers with 5th percentile height and weight whereas the arm
length dimensions are based on the 50th percentile functional arm length
(British industrial male population).
' The data are presented in the form of isobars of equal external force,
and are applied by determining the pathway of a lift through these isobars,11 adopting the lowest force indicated as the safest force for that particular
manoeuvre. Due to the wide variety of postures and lifting which man can
adopt, those covered by the published data are necessarily limited. They
cover a number of one-handed and symmetrical two-handed manoeuvres, all
executed with a straight back. Stooping is deliberately excluded to avoid
any suggestion of acceptability for this lifting posture. However, postures
such as may be adopted during kinetic lifting, which may involve a non-erect
10
back, are also omitted. The data set assumes lifting in unrestricted space,
and a lifting rate of up to once per minute (Materials Handling Research
Unit, 1980). Bates up to six per minute are covered by a reduced loading
limit of 70% of those for less frequent lifts. This limit is not derived
from fatigue effects on the IAP, but on heart rate and 'other physiological
measurements' (Davis and Stubbs, 1978b). Legg (1981) reported a study of
the effects of fatigue and training on 1AF levels during lifting tasks.
Neither parameter was found to influence 1AP levels and it was concluded
that any increased risk of back injury due to abdominal muscle fatigue would
not be mediated via IAP changes.
A subsequent paper from the Materials Handling Research Unit (Davis,
1981) indicates that the data set on which these contours are based has a
typical coefficient of variance of over 32%. For a 5th percentile IAP of
90 mm Hg, the 50th percentile pressure would therefore be of the order of
58 mm Hg, indicating the conservative nature of this limit.
The requirements for symmetrical lifting of evenly balanced objects,
and the erect postures covered, reduce the general applicability of these
lifting limits to industrial tasks. Ridd (1983) presented data on the
effects of spatial restraints on intra-abdominal pressure. The author
examined the effects of a number of factors including reduced headroom and
asymmetrical lifting. None of the tables of data has standard deviations
associated with the means and no statistical significance is attributed to
any of the differences. The asymmetrical lifting data were equivocal. In
free space, most mean pressures quoted were higher than those for
symmetrical lifts with a typical pressure increase of 11%. However, with
reductions in available headroom down to 80% of stature, the asymmetrical
lifts showed a slight tendency to produce lower pressures (typically 2%
down). Further bending to a fully stooped posture again produced increases
in the IAP relative to the symmetric lift, with an average increase of 16%.
Symmetrical lifting in reduced headroom produced a reduction in lifting
capacity as evidenced by an increase in 1AP for a given lift. Under a
ceiling height equivalent to 90% of the individuals stature, lifting
11
capacity was reduced to an average of 42% of the restricted load with little
further change with any additional reduction in headroom.
Graveling (1984) in a literature review on forces in awkward postures
concluded that there was a considerable degree of similarity in the data for
reduced headroom situations derived in different ways using differing
criteria and went on to produce composite guidelines largely using the more
complete data set based on 1AP criteria but backed, where possible, by
corroborative values from other sources. However, the limited data which
are available for restricted headroom/awkward postures made this a
comparatively limited exercise.
Such a compromise approach forms the essential basis of the N10SH
guidelines discussed below. An alternative approach which could be adopted
would be to carry out direct measurements of the 1AP changes associated with
different mining manual handling tasks. However, the documentation of the
experimentation which resulted in the selection of 100 mm Hg, as the
critical level is not very clear. Stubbs (1973) observed the postures
associated with various occupations in the construction industry, and
subsequently simulated the most frequently occurring lifting postures in a
laboratory. No information was given in this document relating to the
actual IAP values recorded during these studies. Details of quantification
were limited to a comparison of lifting manoeuvres such as:- lift A resulted
in 20 - 25% higher truncal stress than lift B. In addition, the nature of
the subjects who participated in these laboratory studies was not stated.
Davis and Stubbs (1978b) gave more information on these studies, concluding
that those at risk were those 'sustaining repeated, frequent high-trunk
stresses inducing peak intra-abdominal pressures above 100 mm Hg'. This
paper was actually presented in 1976, and in 1977 this conclusion was
modified to an increased liability in 'occupations in which peak intra-
truncal pressures of 100 mm Hg or more are induced'. (Davies and Stubbs,
1977a). This shift of emphasis from frequent peaks above 100 mm Hg to what
is subsequently interpreted as any peaks above this level is not
substantiated either by reworking of the original data or by the
presentation of additional data.
12
A subsequent publication (Stubbs, 1981) quoted some actual 1AP values
from the laboratory simulations carried out as part of the construction
industry study (Stubbs, 1973). Data are only published for full stoop
lifting of 3, 15 or 25 kg weights through distances of 0.42, 1.11 and
1.53 metres. Twelve readings, from an unspecified number of subjects were
reported for each lift, with a maximum of 50% of peaks exceeding 100 mm Hg
(stoop lifting 25 kg through 1.53 m) and a minimum standard deviation of 42%
of the mean. It is apparently this series of readings which was used to
formulate the 100 mm Hg limit. In this paper, the author repeated the
earlier statement relating back injury to repeated, frequent peak IAP values
in excess of 100 mm Hg. However, a further publication from the MHRU
(Nicholson, Davis and Sheppard, 1981) identified tasks on the basis of any
peaks over 90 mm Hg, including several where well under 10% of all peaks
exceeded this level.
Given the questions concerning the validity or precise interpretation
of the 100 mm Hg criterion, absolute assessment of lifting tasks using
direct measurement may not be appropriate. However, comparative evaluations
of alternative lifting conditions using IAP as an objective index of truncal
strain may provide useful information and should be considered further.
In conclusion, a limiting criterion based on intra-abdominal pressure
has been proposed for the assessment of manual handling tasks. The
derivation of this criterion level of 100 mm Hg is not at all well
documented for such a fundamental statement, and appears to be based on a
rather small, highly variable data set. In addition, it is not particularly
clear whether it should be interpreted as an absolute limit, ie no loads
producing peak IAF values in excess of 90 or 100 mm Hg or whether the limit
should be on the frequent occurrence of such peaks. Furthermore, leaving
aside the validity of the criterion on which they are based, the force
limits derived from IAP values have only been produced for a series of
highly stylised postures, and may only be of limited utility in assessing
mining manual handling tasks. However, there may be some advantage in
investigating the use of IAP as an objective measure of truncal load.
13
2.1.3 Electromyography and muscle strength
Andersson et al (1977) studied intradiscal and intra-abdominal
pressures in conjunction with a third measure, electromyography (emg), in
an examination of spinal loading and posture. It was found that all three
variables responded systematically to changes in postures and load, although
the variability of emg and intra-abdominal pressure was high. Intradiscal
and intra-abdominal pressures each showed a significant linear relationship
with the sine of the angle of flexion. The emg recordings were more
complex, and the relationship varied according to the spinal level from
which the measurements were made. Full wave rectified and averaged
electromyographic signals were used for quantitative analysis. Recordings
were made from the trapezius and from the levels of the fourth and eight
thoracic vertebrae (T4 and T8) and the first, third and fifth lumbar
vertebrae (Ll, L3 and L5). Recordings from the trapezius were found to
reach a maximum of 10° of flexion and subsequently to decrease. 14, T8, Ll
and L3 values reached a maximum at 40° and decreased at 50°. L5 values
increased with increasing angle up to the maximum studied of 50°. The three
parameters were also studied when the angle of flexion was held constant at
30° and the external load increased. Both pressure values showed a
statistically significant linear relationship with the external load. Emg
values also increased with greater external load but no statistical
relationship was reported. A given load was found to produce its greatest
effect at higher levels on the back, with the greatest increase in
electromyographic activity from the trapezius.
Two other aspects of posture were also studied. These were lateral
flexion and a combination of spinal rotation and flexion. These were
examined in conjunction with asymmetric loading. Consistent differences
were found between different levels although no statistical analysis was
reported. The changes were not studied in such detail as those reported
above, with only one angle of flexion (20°) being adopted. Lateral flexion
was found to Increase both intradiscal and intra-abdominal pressure and to
vary according to whether the trunk was bent towards or away from the load.
A similar laterality was observed with the emg recordings, with the
trapezius and thoracic area showing greater values on the ipsilateral side
14
whilst, with the electrodes placed in the lumbar region, higher values were
found on the side contralateral to the load.
As with the disc pressure, and to a certain extent with intra-abdominal
pressure, studies have been reported on the relationship between predicted
muscle contraction forces and the myoelectric activity of the muscles
involved. Schultz et al (1982) reported a 'slightly non-linear1 regression
equation with a correlation coefficient of r = 0.992. The curvilinear
nature of the relationship was apparently related to alterations in trunk
angle. The authors reported that less myoelectric activity was exhibited
per unit calculated muscle force when the trunk was flexed than when it was
upright. Thus, when the 12 pairs of data were divided into two groups of 6
(trunk flexed and trunk upright) the best fit lines were linear in each
case, with correlation coefficients of r = 0.976 and r = 0.987 respectively.
There has also been considerable interest in the quantification of
muscle fatigue through the use of the frequency shift phenomenon (Graveling
et al, 1980) although it does not appear to have been used in the
formulation of lifting criteria.
Criteria based on muscle function have however been derived from
studies of muscle strength. Poulsen and Jorgenson (1971) examined the
relationship between the isometric strength of the back muscles and the
maximum weight which an individual could lift. No information was given
regarding how the maximum lifts were determined although it appeared that
bent leg lifting was used. Linear regressions were obtained for men and
women with correlation coefficients of 0.72 and 0.78 respectively.
Simplified forms of the regression lines were then used to calculate
recommended lifting limits for a normal population, using standard muscle
strengths published by Asmussen and Heeboll-Nielson (1961). Three sets of
values were calculated for males and females of various body heights and
weights. These were: maximum lift, calculated from the simplified
regression line, permissible single lift (70% of maximum), and permissible
repeated lift (50% of maximum). The 70% level was selected on the basis of
a visual inspection of the graphs which showed that the distribution of data
round the line went down to about 70% of the predicted values. A more
15
recent publication (Poulsen, 1978) repeated the experimental data, and re-
presented the lifting limits. In this paper, the maximum lifts were derived
from the regression values minus two standard deviations, which conveniently
also came to 30%. The 50% 'repeated lifts' value was based on a previous
publication (Molbech, 1963) which indicated that a frequency of 6 to 10
lifts per minute could be endured for at least 10 minutes if the load did
not exeed 80% of the maximum. Poulsen and Jorgensen interpreted this as 80%
of their maximum permissible (ie 70% of the predicted maximum) and rounded
the values (56% of maximum) down to 50%, to be applied for rates up to 6 per
minute for a short period of the working, day.
Poulsen (1978) did not repeat the frequent lifting category. This
latter-paper did however give more detail on the determination of the
maximum lift values. Each individual was presented with a box of
unspecified.size, loaded with the estimated maximum load for that
individual, minus 5 kg. No information was given on the manner of
estimation. Subjects adjusted the load to determine that which could just
be lifted from the floor to an upright position using 'the knee-action
technique*. This and the back strength measurements were made on a total of
50 people (25 men and 25 women).
Carlsoo (1978) included the measurement of back muscle strength in a
study of the relationships between lifting capacity and various muscle
function tests including electromyography on selected muscle groups. As
with the previous study by Poulsen and Jorgensen (1971) a good correlation
was reported between back strength and lifting capacity, in this case using
any lifting technique. Lifting capacity was determined by progressively
.increasing the weight of 'a box* until the subject's lifting limit was
/reached. No data were presented as only approximately 50 of an intended 150
''subjects had been assessed. One of the interesting features was the wide
variety of muscle activity and coordination (as indicated by the emg
recordings) during both the relatively controlled back and abdominal
strength tests and in the 'free-style* lifting tests. Although no evidence
was presented in this paper, it is conceivable that muscle coordination
rather than muscle strength per se may be the determining factor, with
16
relatively uncoordinated lifts predisposing to back pain and other lifting
problems.
Pytel and Kamon (1981) also studied the utility of strength as a
predictor of lifting capacity. In addition to static back extensor strength
which was measured in the same manner as used by Poulsen and Jorgensen
(1971) static elbow flexor strength, and dynamic lift, back extension and
elbow flexion strengths were determined. A tote box (45 x 30 x 12 cm) was
used for the determination of maximum dynamic lift and maximum acceptable
lift. In both cases, the box weight was adjusted by the subject, in the
first case to the maximum which they could lift and in the latter case to
the load which they considered to be comfortable to lift at a rate of 6 per
minute for a regular work day. The equipment for the determination of
dynamic strengths (Mini-Gym) allowed control of the speed of movement. Two
speeds were used, 0.73 and 0.97 ms . No rationale was given for the
selection of these speeds.
Static back or elbow strengths were not used as correlates on maximum
dynamic lift (MDL). However, linear regression equations and coefficients
were given for MDL on each of the dynamic strength tests. For men, the best
correlation was achieved between MDL and dynamic lift strength (DLS) at a
speed of 0.73 ms (r = 0.87) with all other coefficients being 0.65 or
less. The tests on women gave much higher correlation coefficients on all
comparisons, varying from a maximum of 0.96 (dynamic back extension strength
at 0.73 ms ) to 0.68 (dynamic elbow flexion strength at 0.97 ms ). No
comment was made on this sex difference. In both sexes, tests at 0.73 ms
produced consistently higher correlation coefficients than the equivalent
test at 0.97 ms . All the test results at this speed were therefore
combined to produce a multiple regression equation predicting MDL,
incorporating a factor for sex with a value of one for men and two for
women. However, this equation produced only a marginally higher correlation
coefficient than a much simpler equation only involving dynamic lift2 2
strength and sex. (R = 0.948 cf R = 0.941). The authors concluded that
although this latter equation (MDL = 295 + 0.66 (DLS) - 148 (SEX)) was only
derived from a small group of subjects (10 male, 10 female), the values
obtained compared favourably with a number of other published studies and
17
were therefore considered to be reliable. The equation was intended for use
in individual assessment, and no attempt was made to derive population
norms•
Garg and Ayoub (1980) compared the limits published by Poulsen and
Jorgensen (1971) with others from Martin and Chaffin (1972) and Asmussen et
al (1965). The limits recommended in the former paper were substantially
higher than those from the other two. For example, the 95th percentile
lifting capabilities from Martin and Chaffin for a similar lifting distance
(which should be comparable with the maximum minus two standard deviations
of Poulsen and Jorgensen) are 2 kg lower than the lightest limiting value
specified for any age group by Poulsen and Jorgensen. Similarly, the
repeated lifting values calculated by these authors are consistently higher
than values calculated by Asmussen et al (1965). This difference appears
superficially to be accounted for by a difference in the manner of
calculation, for the former limits are based on 50% of isometric back
strength whereas Asmussen et al used 40% values. However, despite the fact
that the Poulsen and Jorgensen values are derived from figures published by
Asmussen (Asmussen and Heeboll-Nielson, 1961), recalculation of maximum
strengths from the percentage values give maxima from Asmussen et.al
of 2.5 - 4 kg less than the lower end of the ranges cited by Poulsen and
Jorgensen. It appears therefore that several sets of lifting limits have
been derived, based on lifting strength, but that there are considerable
differences between them. There appears to be no justification for
selecting any one in preference to any of the others.
2.2 Psychophysical Criteria
Two main groups of research workers have published lifting limits in
recent years based on the psychophysical criterion of an acceptable lift.
These are the group led by Snook (eg Snook and Irvine, 1967; and
Snook et al, 1970) whose findings have been collectively published as Snook,
1978, and a group from Texas Tech University led by Ayoub (eg McDaniel,
1972; Dryden, 1973; and Knipfer, 1974). The data obtained by Snook and his
co-workers have been used to provide selected percentile ranges of
acceptable lifting weights for a number of different variables whereas those
18
data obtained by Ayoub and his colleagues have been used to prepare
predictive equations. These two approaches will be described in turn.
Both groups used the same fundamental approach to the experimental
protocol in that the subjects were instructed to adjust the workload to the
maximum amount that they could perform without strain or discomfort and
without becoming tired, weakened, overheated or out of breath.
Snook (1978) published maximum acceptable weights of lift, lower, push,
pull (initial and sustained) and carry, for 90th, 75th, 50th, 25th and 10th
percentiles of industrial male and female populations. Lifting and lowering
variables reported were: range of lift (floor to knuckle, knuckle to
shoulder, shoulder to arm reach), frequency of lift (one every five seconds
to one per eight hour period), vertical distance of lift (25, 51 and 76 cm)
and width of object away from the body (36, 49 and 75 cm). All values were
derived from lifting and lowering a regularly shaped evenly loaded box with
good handles. It was further reported that heat stress (30.3°C dry bulb and
65% relative humidity, 26.7°C ETA) reduced the acceptable lifting workload
by 20%. Object length was not reported as a variable as it was not found to
have a significant effect on weight lifted within the range 57 to 89 cm.
Similarly, age was not included as a variable but incorporated into the
percentile values, as results for three ages (20 -30, 30-40 and 40-55) did
not yield any significant differences. Although, as with all studies of
lifting, this series of studies was limited by the use of regularly shaped
objects in good.lifting conditions, the results have several advantages over
those from a number of other studies. In particular, these include the
diversity of lifting ranges and frequencies covered by the data, and the
fact that the participating subjects were allowed a free style of lift.
Ciriello and Snook (1983) reported a further series of psychophysical
studies designed to confirm or reject some of the assumptions made in
interpolating between data points during the earlier studies. The authors
drew attention to an apparent over estimation by 10-15% of acceptable lifts
for female subjects in the earlier work. However, although previous
estimates for females had been too high, a comparison of the results for
males from the two series of studies indicates that the values in the
19
earlier studies were consistently lower, sometimes by as much as 20%, than
those reported by Ciriello and Snook. Although part of the difference may
be accounted for by comparing mean values against 50th percentiles, the
differences are too large for this factor to have had much influence.
The authors also reported oxygen consumptions for a selection of the
faster lifting tasks. These generally exceeded the NIOSH criterion of
1.0 litres min~ for an 8 hour day (NIOSH, 1981) indicating that the
psychophysical technique produced overestimates when assessed against
physiological criteria.
Mital (1983) also concluded that the psychophysical technique produced
overstimates of acceptable lift from a study specifically designed to verify
the psychophysical approach. In the first part of the experiment, subjects
were randomly allotted a task from a selection of frequencies, box sizes and
heights of lift (36 different combinations, 10 subjects!). No indication
was given of the actual lifting tasks used. The subjects then estimated
their acceptable load for an 8 hour shift in the usual way. In the second
part of the experiment, subjects actually worked an 8 hour shift, starting
with the previously selected load but adjusting it if they so wished. It
was found that, by the end of the 8 hour shift, subjects were only lifting
an average of 65% of their starting load.
Although derived in essentially the same manner, the data obtained by
Ayoub and his colleagues (collectively published as Ayoub et al, 1978) were
primarily used in a totally different fashion; the acceptable lifting loads
obtained, together with selected individual characteristics, being used to.' •'•'.*"•obtain predictive equations for acceptable lifting loads. However, even the
simplest predictive equations, with average error ratios ranging from .0966
to .4435, require the determination of back strength and leg strength, and
are not therefore immediately applicable to an industrial task.
Ayoub et al, (op cit) did however use their data to produce a limited set of
percentile values of lifting capacity based on 'repeated, continuous lifting
tasks'. No detail was given on the rate of repetition. Because of this,
comparisons between these data and those published by Snook is difficult.
Ayoub (1977) carried out some comparisons of the data by his own group and
20
that published by Snook and his colleagues. These comparisons were based on
the original papers (eg Snook et al, 1970) rather than the collective tables
which may account for the discrepancy in lifting capacity reported. Ayoub
cited a value of 24 kg from Snook et al (1976) as the lifting capacity for
an average male, lifting at a rate of 1 lift min from floor level to a
height of 50-75 cm above the floor, compared with a value of 27.6 kg from
his own data. However, an examination of the data in Snook (1978) gives a
range of loads varying from 22-30 kg depending on box size and actual
distance lifted (the extremes of the lifting range produced a 1 kg
difference in acceptable load). Comparisons of the effect of lifting
frequency showed a slower decrement of acceptable load with increasing
frequency from the data by Snook than from those by Ayoub for floor to
knuckle and knuckle to shoulder lifting ranges, but that the ranking was
reversed for lifting from shoulder height to reach. Given the increased
risk to health of lifting above shoulder height then the more conservative
data of Snook may appear to be more acceptable.
In obtaining their data, Snook and his colleagues allowed individuals
to select their own preferred lifting technique whereas no reference has
been found in the publications of Ayoub and co-workers to the lifting style
adopted in their studies, although Garg and Saxena (1979) suggested that the
initial (unpublished) reports (McDaniel, 1972; Dryden, 1973 and Knipfer,
1974) were based on a single (unspecified) lifting technique. Garg and
Saxena reported a study in which a psychophysical methodology was adopted to
determine maximum work loads at four different lifting frequencies (3-12
lifts min ) using two specified lifting techniques (bent knee/straight back
and stooped) and free style lifting. The mean acceptable work load was
consistently higher for free style lifting for all four lifting frequencies,
ranging from 4.8 to 15.6 kg m min higher (stooped back was also
consistently higher than bent knee). No Indication was given regarding the
style of lift being adopted during the free style lifts. Differences of
this magnitude (8-30%) could account for the differences in lifting capacity
as determined by Snook and Ayoub. It is not possible to determine whether
the differences were genuine, or an artefact of the relative inexperience of
the subjects in one or other of the imposed methods of lifting. The six
subjects used were college students who were reported as having had 'some
21
previous experience in manual materials handling jobs'. This finding
illustrates a conflict between different assessment criteria. Lifting with
a stooped back is regarded as unsafe on biomechanical calculations because
of the forces generated in the lower spine. However, this and other studies
have shown workers to be willing to lift more in this fashion than with a
straight back/bent knee technique, presumably finding it easier.
These psychophysical criteria, particularly those of Snook and his
colleagues have an intrinsic appeal as loads which individuals find to be
acceptable. They are largely derived from industrial populations (unlike
many studies) and did not entail the imposition of unaccustomed lifting
practices. Within.the limitations of the handling situations studied they
provide comprehensive, comparatively easily applied assessment criteria.
However, the more recent papers by Ciriello and Snook (1983) and Mital
(1983) must cast some doubt on their validity. Arguably, the exceeding of
physiological criteria may be as much a reflection on the validity of these
criteria which, as indicated in the next section, are far from unequivocal.
However, the finding by Mital of an overestimation when tested against an
actual 8 hour shift causes more concern. Furthermore, as stated above, the
criteria are restricted to smooth, two-handed, symmetric lifting of
regularly shaped objects in good lifting conditions and therefore are
unlikely to be particularly appropriate in many industrial contexts.
2.3 Metabolic Criteria
In repetitive lifting the critical factor generally ceases to be
primarily muscular strength or the tolerance of other body components to
the biomechanical forces involved. Lifting tolerance becomes a function of
the ability of a particular individual to maintain an adequate oxygen and
thus energy supply to the working muscles, generally referred to as the
aerobic capacity or maximum oxygen uptake (Vo. max). Jorgensen and Poulsen
(1974) examined the relationship between oxygen uptake and lifting at
different frequencies. Using four male and four female subjects, the
authors demonstrated a curvilinear relationship between maximum lifting
frequency and relative load, based on an upper physiological limit of 50%
Vo_ max. These data were used, in conjunction with 5th percentile maximum
22
oxygen uptake population norms (mean - 2 sd) derived from Astrand and
Christensen (1964) and equivalent maximum permissible lift values calculated
according to Poulsen (1970), to derive a table of maximum lifting
frequencies for males and females of two ages (20 and 55 years) and two
heights (150 and 170 cm). The data were calculated as permissible maximum
lifting frequencies for different percentages of maximum lift (10, 25, 50
and 75%).
The values obtained are, in one respect, conservative in that both
oxygen uptakes and maximum lifts are based on the lower end of the normal
distribution. However, they are calculated on the assumption of 50% V6_ as
an acceptable work load for a normal shift whilst several authors, eg
Rodgers (1978) have suggested 33% to be a more realistic figure. The
situation is further complicated because values for Vo. max depend on the
manner in which the maximum is determined. Thus Petrofsky and Lind (1978)
drew attention to their observation that Vo. max measured by pedalling a
cycle ergometer (as were those from Astrand and Christensen) was higher than
that determined on lifting tasks. With lighter loads (7 kg) this
differential could be as much as 30%.
Garg and Saxena (1979) adopted a 'physiological fatigue criterion' of
5 Kcal min which is regarded as equivalent to 33% of the Vo? max of a
young, healthy, adult male (Garg and Ayoub, 1980), in their examination of
the metabolic load associated with acceptable loads at different lifting
frequencies as determined by a psychophysical technique. With a lifting
frequency of 3 lifts min , the average load lifted in a free style lift was
approximately 23 kg. However, the metabolic costs associated with this load
and those for stooped or bent knee lifting, were significantly lower than
5 Kcal min ; indicating, as was suggested by the authors, that muscle
strength rather than aerobic capacity appeared to be the limiting factor. A
similar result was observed at 6 lifts min for free style or stooped back
lifting, but not for bent knee lifting (presumably reflecting greater lower
limb strength). At the highest frequency (12 lifts min ) the metabolic
cost of bent-knee lifting was significantly higher than 5 Kcal min and
subjects were willing to lift far less than with other techniques. This was
23
considered to reflect the greater proportion of body weight being raised
with each shift. Free style lifting was found to have the lowest metabolic
cost per unit work, and a frequency of 9 lifts min was most efficient.
The authors did not derive any lifting limits based on their data. They did
however draw attention to the potential errors which could arise if data for
one lifting frequency were extrapolated to others.
Lind and Petrofsky (1978) examined the relationships between aerobic
capacity (Vo_ max) and fatigue in more detail. They found that fatigue
occurred above approximately 50% Vo. max (±10%) as measured for that lifting
load. This was regarded as an Important consideration because, for example
in lifting light boxes (7 kg), fatigue could occur at work loads greater
than 33% of the Vo. max as determined on a cycle ergometer.. j- - ,
Garg and Ayoub (1980) published a figure illustrating the effect of
lifting technique on physiological cost based on regression equations
published by Garg et al (1978). The figure showed that, for rates above 5
lifts min , at least twice as much could be lifted at a physiological cost
of 5 Kcal min using the stooped back technique than could be lifted using
a bent knee lift. A comparison of published lifting limits derived
according to psychophysical and physiological criteria (Garg and Ayoub,
1980) showed that those based on psychophysics were lower at low lifting
frequencies and higher at high frequencies.
In conclusion, estimates of the physiological limits which should be
placed on lifting work vary from 30-50% Vo. max. Limits in terms of energy_1 i
expenditures of 4.2 to 5.2 Kcal min have also been suggested (Astrand and
Rodahl, 1977; Garg et al 1978) which, from data published by Astrand and
Rodahl (1977) appear to be approximately equivalent. Some of the
"disagreement between authors may be a function of the manner in which the
maximum oxygen uptake (aerobic capacity) is determined, and it has been
suggested (Petrofsky and Lind, 1978) that the higher values are correct if
maximum aerobic capacity is determined for the task under examination rather
than on a cycle ergometer.
24
Snook et al (1970) suggested that whereas muscle strength was the
limiting psychophysical factor for lower frequencies/higher loads,
physiological fatigue was the dominant factor at higher frequencies/lighter
loads. However, although the observations of Garg and Saxena (1979) cited
above support this theory for lower frequencies, the influence of
physiological fatigue at higher lifting frequencies is more complicated.
Thus Lind and Petrofsky (1978) reported local muscle fatigue as a limiting
factor with low loads/high frequencies. The same authors published values
for extended work (4 hours) which showed subjects working at an average of
54% (±7%) of their aerobic capacity measured on the same task. This was
equivalent to an oxygen consumption for these subjects of 1.65 litres min
or an energy expenditure of 8.25 Kcal min , substantially above the 5 Kcal
min limit cited above. A limit of 50% Vo_ max may well therefore be a
realistic limit for repetitive, moderate weight lifting although for
heavier, less frequent loads or very light rapid lifting, local muscle
fatigue may restrict safe lifting capacity below such a limit. However, the
application of such a limit to industry would require the determination of a
lengthy series of task related 'norms' for aerobic capacity.
3. A 'HYBRID' CRITERION
NIOSH have recently published a work practices guide for manual lifting
(NIOSH, 1981). This examines lifting limits based on epidemiological
(injury rates), biomechanical (spinal forces), metabolic and psychophysical
criteria, and develops a hybrid series of limits based on these. It does
not make use of the limits derived by Davis and Stubbs (1977 et seq)
although it does briefly refer to them. The limits are divided into three
zones': (1) 'Acceptable Lifting Conditions', which is divided by the 'Action
Limit1 from 2) 'Administrative Controls Required1 within which either
administrative (personnel selection or training) or engineering (job
redesign) controls are required. This in turn is separated from the
'Hazardous Lifting Conditions' zone by the 'Maximum Permissible Limit*. The
Hazardous Lifting Zone is regarded as hazardous to any individual and such
jobs require engineering controls.
25
The three zones are defined by equations representing the Action Limit
(AL) and the Maximum Permissible Limit (MPL).
AL (Kg) = 40 (15/H) (1 - .004 (V - 75 )) (.7 + 7.5/D) (1 - F/Fmax)
MPL - 3 (AL)
where H = horizontal location (cm) forward of midpoint between
ankles at origin of lift; 15 = H = 80
V = vertical location (cm) at origin of lift; 0 = V = 175
D = vertical travel distance (cm) between origin and
destination of lift; 25* = D• - 200-V
F = average frequency of lift (lifts min ); .2 = F = max
0F = maximum frequency which can be sustainedmax
* For travel < 25, D - 25
+ For frequency < .2, F = 0
0 F varies with V and lifting periodmax
The Action Limit Loads can be safely lifted ('represents nominal risk1)
by over 99% of men, the MPL by 25%. The equation for the AL does not
require any data regarding the workforce. As F approaches F , the
frequency component in the equation approaches zero. Therefore, at F ,1 maxAL =-0 ie the equation does not consider any lifting at a frequency of F
-1 -i(12-18 lifts min ) to be acceptable. Varying lifting rates below 1 min
has little effect on AL as F approaches 1 at such rates.
A comparison of the Action Limits obtained using the equation with the
limits published by Snook shows some interesting differences. In the
26
examples the data of Snook (1978) have been extrapolated to the 99th
percentile (2.576 s.d. assuming a normal distribution) to facilitate
comparison with the NIOSH values. At all but the fastest.rate cited by
Snook (12 lifts min ) the NIOSH equation gives a much higher lifting limit
for lifting a compact object from the floor to knuckle height (typically
approximately 15 kg greater), a pattern which is repeated for shorter
lifting differences. However, with a larger object requiring to be held
further away from the body (hands 38 cm away rather than 18 cm away) the
values published by Snook are higher by 2-3 kg. A similar pattern emerges
with lifting in higher lifting zones (shoulder to reach) although the
differences are less marked (seldom more than 7 kg) and the faster lifting
rates follow the general pattern.
The NIOSH criteria apparently therefore place greater emphasis on the
biomechanical stresses imposed on the body, in particular the spinal cord,
when the centre of gravity of a load acts further away from the body, than
do the psychophysical limits developed by Snook. The latter limiting values
are referred to as acceptable limits rather than safe limits and it is
conceivable, particularly considering the insidious onset of much back pain,
that workers would be willing and able to lift loads which may have a
detrimental long-term effect on spinal discs or other structures associated
with the development of back pain.
The equations published by NIOSH are only applicable to smooth, two-
handed symmetric lifting in the sagittal plane, with good lifting
conditions. No reference is made to presumed level of training although the
workforce is assumed to be physically fit and accustomed to physical labour.
However, as training is specifically referred to as a form of administrative
control, it appears that no initial training is presupposed. No Indication
is given regarding the presumed effectiveness of subsequent training. Thus,
if the characteristics of a particular task fall between the AL and the MPL
indicating that administrative controls could be used, there is no way of
determining whether lifting training, in accordance with the procedure
defined in the NIOSH guidebook, can be regarded as rendering that task safe
for the trained workforce.
27
4. HEALTH AND SAFETY COMMISSION; REGULATIONS AND GUIDANCE
The Health and Safety Commission have published a consultative
document containing proposals for regulations and guidance on the manual
handling of loads (HSC, 1982). The draft regulations prohibit the manual
handling of any load likely to injure an individual because of '(a) its
weight, shape, size or lack of rigidity; or (b) the frequency with which he
handles loads; or (c) the conditions under which the load is to be handled*.
To facilitate compliance with these regulations the HSC have published a
guidance document which is intended to identify the sources of risks and
hazards involved in manual handling and to provide guidance about positive
steps which can be taken to minimise these risks. However, this document
has since been considerably revised and a new consultative document is
expected. It is not therefore appropriate to discuss the previous version
in detail.
':. V;- V
5. CONCLUSIONS
Many different limits to lifting have been proposed, based on a variety
of criteria. With the exception of the data reported by Ridd (1983), they
are restricted in their application to smooth lifting in good conditions and
are further limited to symmetrical, compact objects. Despite the initial
intrinsic appeal of limits derived on psychophysical principles they have a
potential inherent risk in that the epidemiology of back pain would suggest
that workers engaged in manual handling may willingly handle loads which may
be having a long-term detrimental effect. Furthermore, recent papers have
questioned the validity of the limits determined in this manner.
Other sets of guidelines, although based on a common criterion (eg,
-muscle strength), provide conflicting sets of values with no immediate way
==of .determining which, if any, are correct.
The guidelines recently published by the American National Institute of
Occupational Safety and Health (NIOSH, 1981) are a compromise between a
variety of approaches which may remove some of the deficiencies of the
individual methods (although they may equally compound them!). However, in
addition to the fact that they are only applicable to smooth, two-handed
28
lifts, the guidelines have further shortcomings which would require
clarification before they could be usefully employed in industry.
Furthermore, the apparently complex equation may well discourage its routine
industrial use.
The absence of any useable limits suggests that the best approach to
the assessment of manual handling tasks may include some form of direct
measurement of the strain imposed on the body as a result of manual
handling. Although there are reservations regarding the precise validity of
the assessment criterion currently employed (see section 2.1.2), the
measurement of intra-abdominal pressure, if only as a comparative measure,
would appear to be the most immediately practicable in an industrial setting
and worthy of further investigation.
ACKNOWLEDGEMENT
This report was prepared during the joint NCB/ECSC funded project
number 7247/12/014 (An Ergonomics Evaluation of the Haulage and
Transportation of Mining Supplies).
29
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35
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