6.4.1 Much research on human tolerance to acceleration
has been conducted at the United States Air Force Aeromedical Research
Laboratory (AFAMRL) in Ohio. The most extensive work dealt with accelerations
causing compression along the spine'. This is positive +Gz or
"Eyeballs Down" acceleration. Less work has been conducted on accelerations
perpendicular to chest and parallel to the shoulders. This research
has formed the basis of the dynamic response criteria accepted by
IMO.
6.4.2 To determine the injury potential of an
acceleration field, Brinkley and Shaffer (1971) introduced the concept
of the Dynamic Response (DR). The basis of this concept is the supposition
that each body axis can be idealized as an independent single degree-of-freedom
spring-mass system that is subjected to known seat accelerations (Brinkley
and Shaffer, 1984). This model is shown in figure 6.4. It was originally
developed to evaluate the effects of acceleration along the spine,
but has been expanded to evaluate the effects of acceleration perpendicular
to the chest and parallel to the shoulders.
Figure 6.4 Independent Single Degree-of-Freedom Representation of the
Human
6.4.3 The dynamic response is computed by:
where is the undamped natural frequency for the axis studied, δ(t)
is the displacement time-history of the body mass relative to the
seat support, and g is gravitational acceleration. Values for the
natural frequencies in each co-ordinate axis have been found through
research conducted at AFAMRL. These values for a 50th percentile 28
year old male in a fully restrained seat and harness are presented
in Table 6.1
6.4.4 The DR computed with Equation 6.3 represents
an equivalent static acceleration of the body mass in an undamped
system. The peak value of the DR curve is called the Dynamic Response
Index (DRI). It can be used as an indicator of the potential for acceleration
forces to cause human injury.
Table 6.1 Parameters of the
Dynamic Response Model
| Coordinate Axis
|
Natural Frequency (rad/s)
|
Damping Ratio
|
| X
|
62.8
|
0.100
|
| Y
|
58.0
|
0.090
|
| Z
|
52.9
|
0.224
|
6.4.5 Brinkley and Shaffer (1984) defined three
risk levels for acceleration forces directed along the spine. These
risk levels are characterized as high, moderate, and low. They relate
to a 50%, 5% and 0.5% probability of injury, respectively. The 50%
probability of spinal inury is the highest rate observed for USAF
ejection seats. It should be noted that there was no spinal chord
damage associated with these injuries. The moderate risk level, which
is currently used in USAF ejection seat design, is midway between
the high risk and low risk levels. The low risk level corresponds
to acceleration conditions used routinely without incident during
test conducted with volunteers at the AFAMRL. The three injury curves
presented by Brinkley (1985) for the +z axis are shown in Figure 6.5.
Each curve, which represents a constant DRI at the appropriate risk
level, was computed from half-sine acceleration impulses acting at
the seat support. The DRI limits presented by Brinkley (1985) for
each risk level are shown in Table 6.2 .
Figure 6.5 Three Risk Levels For Acceleration Acting In the +Z Axis (Brinkley,
1985)
6.4.6 The risk levels for the ±x, +y, and
–z axes were determined without the benefit of a statistically
based method such as that used for the +Z axis (Brinkley and Shaffer,
1984). The high risk levels were determined by calculating the peak
response of the mathematical model to acceleration conditions known
to cause major injuries or potentially serious sequelae. The low risk
levels were determined on the basis of calculated model responses
to acceleration conditions that have been used numerous times for
noninjurious tests with human subjects in research laboratories. The
moderate injury level was assigned as the midpoint between the high
and low levels. The DRI limits for these axes are presented in Table
6.2.
Table 6.2 DRI Limits for three
Risk Levels
| Coordinate Axis
|
DRI Limits (G's)
|
| High
|
Moderate
|
Low
|
| +X
|
46.0
|
35.0
|
28.0
|
| -X
|
46.0
|
35.0
|
28.0
|
| +Y
|
22.0
|
17.0
|
14.0
|
| -Y
|
22.0
|
17.0
|
14.0
|
| +Z
|
22.8
|
18.0
|
15.2
|
| -Z
|
15.0
|
12.0
|
9.0
|
6.4.7 The response limits presented in Table 6.2
are for single axis accelerations. Normally, components of acceleration
are acting in each co-ordinate direction simultaneously. The effects
of multi-axial acceleration can be evaluated with an ellipsoidal envelope.
The boundaries of the envelope in each direction are the DRI limits
presented in Table 6.2. The seat accelerations to which the occupant
is subjected, then, are limited by:
DRIx, DRly, and DRlz in
Equation 6.4 are the limiting DRI's in the x,y, and z co-ordinate
directions, respectively, for a particular risk level. DRx,
DRy and, DRz are the calculated dynamic responses
of the body mass in the same directions
6.4.8 The number of computations required to evaluate
an acceleration field can be reduced if the apparent relative diplacement
of the body mass with respect to the seat support is used directly
to determine acceptability instead of computing the DR. This approach
is valid because, as shown in Equation 6.3, the DR is a linear function
of the relative displacement.
6.4.9 The displacements permitted by the IMO criteria
are presented in Table 6.3. These allowable displacements were computed
from the DRI limits presented in Table 6.2 and the natural frequencies
presented in Table 6.1. The "Training Condition" corresponds to a
0.5% probability of injury. This was deemed to be the maximum acceptable
for training exercises because these acceleration forces will be experienced
several times. The "Emergency Condition" corresponds of a 5% probability
of injury. This level was deemed acceptable in potentially life threatening
situations.
Table 6.3 Suggested Displacement
Limits for Lifeboats
| Acceleration Direction
|
Displacement (in)
|
| Training
|
Emergency
|
| +X-- Eyeballs
In
|
2.74
|
3.43
|
| -X-- Eyeballs Out
|
2.74
|
3.43
|
| + Y-- Eyeballs
Right
|
1.61
|
1.95
|
| -Y-- Eyeballs Left
|
1.61
|
1.95
|
| + Z-- Eyeballs Down
|
2.10
|
2.49
|
| +Z--Eyeballs Up
|
1.24
|
1.66
|
6.4.10 When relative displacements are used as
the basis for determining the acceptability of an acceleration field,
the effects of multi-axis accelerations can be evaluated with the
Combined Dynamic Response Ratio (CDRR). The CDRR represents a displacement
envelope that is analogous to the acceleration envelope implied in
Equation 6.4. It is computed by:
Sx, Sy, and Sz in Equation
6.5 are the allowable displacements in the x, y, and z co-ordinate
directions, respectively, for a particular risk level. δx, δy and δz are the apparent computed relative
displacements of the body mass with respect to the seat support. The
peak value of the CDRR time-history is called the CDRR Index. A CDRR
Index that is less than or equal to unity indicates the particular
risk level has not been exceeded. When this analysis is performed,
the acceleration data are not filtered. If an acceleration force does
not have a significant influence on the human, it should not have
a significant influence on the response of the model.
6.4.11 Although Brinkley has shown a good correlation
between spinal injury and DRI, experience with Royal Air Force ejections
indicates that the incidence of spinal injury is not as well correlated
with the DRI. Anton (1991) has presented as series of 223 "within
envelope" ejections in which the discrepancy between predicted injury
rate and observed injury rate is very wide. The DRI indicated that
the injury rate should be about 4% but the actual injury rate was
30-50% depending on the type of seat used.
6.4.12 A possible explanation for this is discrepancy
is the type of harness used in military aircraft in the United Kingdom.
The preferred harness type is the simplified combined harness (SCH)
which provides restraint in normal circumstances but becomes the parachute
harness after ejection. The harness is part of the seat equipment.
The torso harness, on the other hand, is favoured by the US forces.
It is fitted to the crew member and worn out to the aircraft where
it is attached to the seat.
6.4.13 The torso harness is recognized to provide
slightly better coupling between the man and the seat. This coupling
is important in reducing "dynamic overshoot," the effect in which
the occupant experiences greater dynamic forces than those applied
to the seat. There is, in essence a second mass spring damper system
operating at the interface between the seat and occupant. This second
spring damper can, however, be incorporated into the dynamic response
model but knowledge of seat coupling and cushion stiffness is necessary.
6.4.14 The effects of seat/occupant coupling,
and the apparent effect of this coupling on observed injury rates,
indicates a strong need for free-fall lifeboats to be equipped with
a properly designed harness system. The issue of harnesses is discussed
later in this paper.