6.4 Dynamic Response Criteria
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Statutory Documents - IMO Publications and Documents - Circulars - Maritime Safety Committee - MSC/Circular.616 – Evaluation of Free-Fall Lifeboat Launch Performance – (22 June 1993) - Annex – Evaluation of Free-Fall Lifeboat Launch Performance - Section 6 – Human Tolerance To Acceleration Forces - 6.4 Dynamic Response Criteria

6.4 Dynamic Response Criteria

  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.


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