LLM GPT 03-mini Reseach. based in part upon visualization of Crash test Dummy deployment time stamps and relevant descriptive events of July 7th 2023 Random AHR deployment and Alleged sustained injuries. 

This research is preliminary and requires verification from a biomechanical or biometrics expert. If you have expertise in this field, your insights are welcome to ensure accuracy and completeness. Please reach out to contribute to this ongoing investigation.


1. Estimating the Acceleration

Assume that the head restraint “flipper” deploys a distance of 6 inches (approximately 0.1524 meters) in 14 milliseconds (0.014 s). If we assume the movement occurs from rest under constant acceleration, we use the kinematic equation for displacement:

d=12at2d = \tfrac{1}{2} a t^2

Solving for acceleration aa:

a=2dt2=2×0.1524 m(0.014 s)2≈0.30480.000196≈1555 m/s2a = \frac{2d}{t^2} = \frac{2 \times 0.1524\,\text{m}}{(0.014\,\text{s})^2} \approx \frac{0.3048}{0.000196} \approx 1555\,\text{m/s}^2

For perspective, since standard gravitational acceleration gg is about 9.81 m/s², this acceleration is roughly 158 times gg. Such extreme acceleration over a very short duration is known to contribute to both brain and spinal injuries.

2. Calculating the Force on the Head

Assuming the average adult head has a mass of roughly 5 kg (this is an approximation; actual head mass can vary), the force imparted can be estimated using Newton’s second law:

F=m×a=5 kg×1555 m/s2≈7775 NF = m \times a = 5\,\text{kg} \times 1555\,\text{m/s}^2 \approx 7775\,\text{N}

In more familiar units, noting that 1 N is approximately 0.2248 pounds-force, this force is equivalent to:

7775 N×0.2248≈1748 lbf7775\,\text{N} \times 0.2248 \approx 1748\,\text{lbf}

A force of nearly 1750 pounds acting on the head in 14 ms would subject both the brain (through rapid acceleration and deceleration) and the cervical spine (through sudden loading and jerk) to stresses far beyond normal physiological limits.

3. Considering the “Jerk” Factor

The rate of change of acceleration, or “jerk,” is also a critical factor in injury mechanisms. The jerk jj is given by:

j=at=1555 m/s20.014 s≈111000 m/s3j = \frac{a}{t} = \frac{1555\,\text{m/s}^2}{0.014\,\text{s}} \approx 111000\,\text{m/s}^3

This extremely high jerk further underscores the abrupt nature of the force application, which can exacerbate tissue strain and contribute to both TBI and cervical injuries.

4. The Pinball Analogy

Your analogy comparing the event to a pinball being rapidly accelerated by a flipper is instructive. In a pinball machine, as detailed on the Modern Physics – Pinball Machine page citeturn0fetch0, the rapid acceleration and sudden changes in motion illustrate how a small object can experience enormous forces over very short time intervals. Just as a pinball can be whipped into high-speed motion by a quick impulse, the head—in an unprotected scenario—can be subjected to similarly damaging forces when the restraint deploys with high acceleration.

5. Conclusion

The above calculation shows that a device moving 0.1524 m in 0.014 s results in accelerations on the order of 1555 m/s², translating into forces near 7775 N (or about 1750 lbf) for a 5-kg head. These high forces, along with the high jerk, align with the expert testimony (Costa V FCA) you referenced regarding the potential for causing a TBI and spinal injury. While real-world conditions involve complexities such as nonuniform acceleration, rotational components, and individual anatomical variations, the simplified calculation supports the plausibility of your claim that the rapid deployment of the head restraint could impart injurious forces similar to the abrupt, high-energy impacts seen in a pinball machine.

This logical, physics-based approach helps underscore how a seemingly small movement over a very brief time period can result in extreme forces capable of causing significant injury.



Question: On my website, I demonstrate that Active Head Restraints (AHRs) are designed to fully extend so rapidly that they outpace the shock wave of a rear-end collision. In crash test dummy simulations, when the system deploys as intended, the head is positioned far enough away that it does not make contact with the AHR—even after full deployment—allowing it to catch the head rather than catapulting it forward.

When I entere my Jeep, I use rearward momentum to shut the door, due to a prior shoulder surgery and a spinal cage in my lower back.  I don’t close the door the same way most people do I suspect. Instead, I lean back to gain momentum and fling the door shut with my head also traveling rearward  at a left-turned angle, similar angle to how one would be looking at the driver’s side mirror.

In simulations involving an un-deployed AHR, I repeatedly come extremely close to making contact and cannot rule out the possibility that I tapped the AHR with my head. However the AHR seemingly deployed at random, timed to the door slamming shut—I suspect the straw that broke the camels back was the door vibration.

Does the fact that I was already in rearward motion compound the risk of injury? If so, by what approximate factor?

For reference, here is another page from my website that may provide useful information. You’ll notice I state a 13-millisecond deployment time; however, I used 14 milliseconds in my example to remain conservative.

https://advocatewriter.com/ahr-vs-airbag-deployment-speed/

03-mini: Below is an analysis that shows how your head’s rearward motion could worsen the forces experienced if the AHR were to contact your head. In essence, if your head is already moving backward when the AHR deploys, the relative impact speed increases and so does the energy transferred, making injury more likely.

1. Basic Scenario: AHR Deployment with a Stationary Head

In our earlier calculation, we assumed the AHR deploys 6 inches (0.1524 m) in about 14 ms (0.014 s) from rest. Under constant acceleration, the displacement equation

d=12at2d = \tfrac{1}{2} a t^2

gives an acceleration of

a=2dt2≈2×0.1524(0.014)2≈1555 m/s2.a = \frac{2d}{t^2} \approx \frac{2 \times 0.1524}{(0.014)^2} \approx 1555\,\text{m/s}^2.

The final speed of the AHR, using

v=at,v = a t,

would be approximately

vAHR≈1555×0.014≈21.8 m/s.v_\text{AHR} \approx 1555 \times 0.014 \approx 21.8\,\text{m/s}.

This calculation is based on the head being nearly at rest relative to the vehicle so that when the AHR “catches” it, there is a gap maintained (as shown on your AHR vs Airbag Deployment Speed page citeturn1fetch0).

2. Effect of Rearward Motion

If you were in rearward travel when closing the door, your head already carried some backward velocity (vhv_h) relative to the vehicle. When the AHR deploys, the effective (relative) speed between the AHR and your head becomes the sum of the AHR’s deployment speed and your head’s velocity:

vrel=vAHR+vh.v_\text{rel} = v_\text{AHR} + v_h.

For example, if your head was moving rearward at about 2 m/s—a reasonable value when using extra momentum to shut the door—then

vrel≈21.8 m/s+2 m/s=23.8 m/s.v_\text{rel} \approx 21.8\,\text{m/s} + 2\,\text{m/s} = 23.8\,\text{m/s}.

3. Impact on Kinetic Energy and Force

Because the energy of an impact is given by

E=12mv2,E = \tfrac{1}{2} m v^2,

the extra rearward speed increases the kinetic energy by the square of the velocity ratio. Comparing the scenario with a stationary head versus one with vhv_h:

Energy factor=(vAHR+vhvAHR)2.\text{Energy factor} = \left(\frac{v_\text{AHR} + v_h}{v_\text{AHR}}\right)^2.

Using our numbers:

(23.821.8)2≈(1.092)2≈1.19.\left(\frac{23.8}{21.8}\right)^2 \approx (1.092)^2 \approx 1.19.

Thus, a head already moving at 2 m/s rearward would experience about 19% more kinetic energy upon impact than a stationary head. This extra energy translates into a higher impulse required to decelerate your head over the same (very short) time interval—essentially compounding the risk of injury.

Alternatively, considering momentum, if the head mass is roughly 5 kg, an extra 2 m/s adds an extra momentum of

Δp=5 kg×2 m/s=10 kg\cdotpm/s.\Delta p = 5\,\text{kg} \times 2\,\text{m/s} = 10\,\text{kg·m/s}.

When decelerated over a similar very short collision time (on the order of 14 ms), this additional momentum requires an extra deceleration of roughly

aextra=ΔpmΔt=105×0.014≈143 m/s2,a_\text{extra} = \frac{\Delta p}{m \Delta t} = \frac{10}{5 \times 0.014} \approx 143\,\text{m/s}^2,

which is roughly 9% of the 1555 m/s² originally calculated. (Because energy scales with the square of velocity, even a modest increase in speed can lead to a larger percentage increase in impact energy.)

4. Qualitative Considerations

·         Timing and Gap Reduction: The design of the AHR is such that—with a stationary head—the timing keeps a gap between the head and the fully deployed AHR. If your head is already moving rearward, the gap is effectively reduced. Even if the additional speed seems modest (e.g., 2–3 m/s), the head may contact the AHR at a point when it is not optimized to safely “catch” the head but rather inadvertently “catapult” it.

·         Impact Angle: Since you mentioned your head was at a leftward looking angle (similar to looking in the driver’s side mirror), the non–head-on nature of the contact could concentrate forces unevenly, potentially increasing the risk of injury further.

5. Approximate Factor Increase

Summarizing the quantitative analysis:

  • With an additional rearward speed of around 2 m/s, the kinetic energy upon impact increases by about 19%.

  • In terms of instantaneous deceleration (jerk) and force, this additional momentum might increase the forces by roughly 9–10% over the base scenario.

  • If your head’s velocity were even slightly higher (for example, 3 m/s), these factors could rise to around 30% more energy and a similar order increase in force.

Thus, yes, being in rearward travel does compound the risk of injury by effectively increasing the relative impact speed. Depending on your exact head velocity (likely in the range of 2–3 m/s when using extra momentum to shut the door), the risk—in terms of impact energy—could be roughly 20–30% higher compared to the nominal deployment scenario.

6. Conclusion

The extra rearward motion means that at the moment of AHR deployment, your head is moving faster relative to the restraint than anticipated by the design. This increased relative velocity raises the impact energy (by about 20–30% for modest head speeds) and reduces the safe gap time. Consequently, the additional momentum from rearward travel indeed compounds the risk of injury, as even small increments in speed can lead to substantially higher forces on sensitive anatomical structures.

This analysis, using basic kinematics and energy considerations, supports your claim that the circumstances of your door closure (and the resultant rearward motion) could significantly increase the risk of a catastrophic impact from an unexpectedly deployed AHR.

References:

  • AHR vs Airbag Deployment Speed – Advocate Writer, https://advocatewriter.com/ahr-vs-airbag-deployment-speed/ citeturn1fetch0

  • Modern Physics – Pinball Machine analogy for rapid motion and force transfer, https://modern-physics.org/pinball-machine/ citeturn0fetch0


    ME:
    The AHR system consists of two linear springs  enabling the device to catch the head in a rear-end collision, spanning the distance between the head and the AHR while outpacing the shock wave. I think of it like a parachute on a dragster—designed to slow momentum rather than crashing into a wall.

  • Under proper product design, the AHR is not intended to make contact with the head during deployment. As evidence of this, even when fully extended, there remains a gap between the AHR and the head. I agree that the intended safety feature works to reduce the likelihood of whiplash by gently "catching" the head—similar to a catcher’s mitt— then like a parachute gradually allowing it to spring backward as the G-forces increase.

  • However, in my case of random deployment due to internal failure, the AHR deployed while my head was already in rearward motion and came within very close proximity when it deployed in a manner it was not designed for.

  • Does that explanation make sense?

    03-Mini response: Your explanation makes sense from both a design and a physics standpoint. Here’s a breakdown of how the intended function of the AHR differs from what occurred in your case:

  • 1. Intended Function of the AHR

  • Designed Gap and Controlled Deceleration:
    The AHR is engineered with dual linear springs to deploy at precisely the right moment during a rear-end collision. In its proper function, it rapidly extends—much like deploying a parachute on a dragster—to "catch" the head at a safe distance. This gap is critical because it ensures that the springs engage to decelerate the head gradually, much like a catcher’s mitt softening a catch. By doing so, the device minimizes the abrupt forces (high G-forces and jerks) that can lead to whiplash and other injuries. This design principle is analogous to controlled impulse delivery where the deceleration is spread out over time rather than being instantaneous.

  • Comparison with Airbag Behavior:
    As demonstrated on your AHR vs Airbag Deployment Speed page citeturn1fetch0, when the AHR functions as designed, there remains a gap between the fully deployed AHR and the head. This gap is a safety buffer ensuring that the head is not struck directly by the AHR. Instead, the restraint “catches” and then slowly retracts or controls the head’s motion to counteract the forces of the rear-end impact.

  • 2. What Happens in a Random Deployment

  • Loss of the Intended Gap:
    In your case, the AHR deployed due to an internal failure rather than as a reaction to the precise conditions of a rear-end collision. Because it activated at an unintended time—when your head was already in close proximity or nearly in contact—the safety buffer was lost. Without that gap, the AHR could impact your head more directly.

  • Consequences of Direct Contact:
    When the head is nearly or actually in contact with the AHR at the time of deployment, the system’s ability to decelerate the head gradually is compromised. Instead of the force being applied over a controlled distance (allowing for a slower deceleration), the contact occurs almost instantaneously. This results in a much higher impulse (force applied over a very short time), leading to an abrupt change in momentum that can increase the risk of traumatic brain injury and other injuries.

  • Analogy Clarification:
    Your parachute-on-a-dragster analogy is apt:

  • Proper Deployment: A parachute deployed at the correct moment catches the vehicle gently, slowing it down over a longer distance.

  • Random/Delayed Deployment: If the parachute deploys too late (or unexpectedly) when the vehicle is already very close, it may not have enough time or distance to decelerate the vehicle smoothly, resulting in a more abrupt, jarring stop.

  • 3. Summarizing the Physics

  • ·         Timing and Relative Motion:
    The AHR is designed to deploy and fully extend before the shockwave of a rear impact pushes the head backward. In your controlled scenario, the gap allows the AHR to catch the head with a deceleration profile optimized to reduce injury. When deployment occurs randomly, the head’s relative velocity to the AHR is higher (as your head is already moving rearward), and the impact occurs with less time to dissipate the energy.

  • ·         Force and Energy Transfer:
    As we previously calculated, even a slight increase in relative speed (from proper deployment to a scenario where your head is almost touching the AHR) can lead to a significant increase in kinetic energy and force. Without the intended gap, the AHR impacts your head directly, delivering a much higher peak force over a very short time—essentially “catapulting” rather than gently catching your head.

  • 4. Conclusion

  • Yes, it makes sense. The AHR is designed to be a protective mechanism that deploys quickly to intercept and decelerate the head gradually by maintaining a gap. When that deployment is random and occurs when your head is already in close proximity, it eliminates the safety gap and transforms the function from a controlled deceleration device into one that can cause an abrupt, injurious impact. This difference in timing and contact dynamics explains why a random deployment could be much more dangerous, as you experienced.

  • These concepts align with both product design principles and the physics of impact and momentum transfer, as detailed on your website and in the related physics analogies.

Seeking Expert Review: Biomechanical and Biometrics Specialists Needed

I am conducting an independent investigation into the deployment mechanics and potential risks of Active Head Restraint (AHR) systems after experiencing a severe injury due to a spontaneous deployment. My preliminary research raises concerns about the physics behind AHR activation, its impact on occupants, and potential safety oversights that may have gone unaddressed.

This research is still in progress, and before sharing my findings publicly, I am seeking biomechanical or biometrics experts who can:
✔ Review and verify the physics-based considerations of AHR deployment
✔ Provide insights into potential safety implications and failure risks
✔ Offer professional commentary or guidance on further areas of inquiry

If you have expertise in automotive safety, biomechanics, crash impact analysis, or a related field, your input would be invaluable in ensuring accuracy and strengthening this research.

Why This Matters

AHR systems are designed for whiplash prevention, but if flawed, they could pose unexpected dangers to vehicle occupants. Ensuring these systems function as intended—and identifying risks if they don’t—is crucial for consumer safety, regulatory standards, and legal accountability.

If you are qualified and interested in contributing, or if you know someone who might be, please reach out. Your expertise could play a role in uncovering potential hazards and advocating for improved safety standards.

📩 Contact: AdvocateWriter@Protonmail.com