Hard Opening

To begin that process, we must first understand all about opening shock. When we talk about hard openings, we must delineate between types. There are openings which merely deflate your lungs, and there are openings which do serious physical damage to you and/or your gear.
We will concentrate on the latter while trying to cover the complete spectrum. Before we go into the technical part of this article, something must be said about jumper perception of opening shocks. This is best illustrated by relating a conversation with an old friend who was doing some test jumping for another parachute company. He spoke about making a jump one day with a data logger to record force and getting a normal opening shock. Using the same pack job and again with a data logger made a jump the second day and it slammed him. The data from both jumps showed the same relative force, but the jumper felt the second jump was much harder. This is largely due to preparedness or lack thereof, of the body and mind before deployment. It is due to the way you feel on a given day and is not what we are looking for in terms of analysis of potentially destructive openings. Opening shock can be divided into basic components: “Snatch Force” and “Inflation Force”. Snatch force is that point in the deployment when the mass is accelerated to speed. This simply means when everything (lines, canopy, and bridle) is stretched out with tension and load. When that load occurs, you are at snatch. This is also when the slider is beginning to take air. Hopefully the slider won’t take air until just after snatch. This can be helped by rubber banding the apex of the slider to a center B or C line attachment to momentarily retain it. Inflation force, on the other hand, normally occurs after snatch and has less force than snatch. It is when the canopy begins inflation and commences the argument between the resistance of the slider and the inflation forces spreading the canopy. This usually occurs in steps of decreasing force.
Deployment Bag design: The D-bag is the single most important component in this equation. There is much conversation and disagreement about this subject. Here is my take. The D-bag is used to prevent the canopy from taking any air or opening prior to an orderly, properly sequenced line deployment. We use the suspension lines stowed in rubber bands to keep the bag closed. There are other devices designed to do the same job, and the phenomenon described here is applicable to all of those devices. If the bag is allowed to open prematurely, exposing the canopy to inflation, you will have a very hard “canopy first” opening. These openings may vary in intensity depending on exactly when in the process of deployment the canopy inflation begins. We want inflation to be the last thing that happens. This malfunction is referred to as line strip/dump or “out of sequence deployment”.
What causes the lines to release from the bag, allowing the canopy to get out prematurely? Inertia is the answer. Newton said, “Bodies at rest tend to stay at rest; bodies in motion tend to stay in motion. A body is a unit of mass. Lines stows are divided into 3 units of mass. They are: the bights 2 each, and the span, or the part of the lines between the stows or bights. Each of these components, separated by the stow rubber bands, is a unit of mass within itself. The mass of the 2 bights must equal the mass of the span. In terms of percentage, the span should make up 50% of the entire line stow from side to side. We want 25% in each bight so as to equalize the tendency of the span to “drop out” or “Dump” or “Strip” or pull the bights out of their stows upon extraction from the container, by overcoming their mass. The combined mass of the bights equalizes the downward force of the span portion of the lines as they try to stay in the pack tray upon bag extraction. If the mass of the span is greater than the mass of the bights, then it will pull the bights out of the stows upon extraction from the container. If the span is, say, 70% of the entire line stow from side to side, that only leaves 30% to be divided by each bight, or 15% per side. The 70% in the middle will easily overcome the 15% on each side.
Most severe openings occur at high speeds. The higher the Dynamic Pressure, or “Q,” the more things drag and the greater the differential of mass inertia. In order to endure these forces, the deployment must be smooth and progress evenly throughout the process. The spread of your arms in freefall will do more to change the nature of the opening than any normal pack job. In other words, slow down when you deploy; it will soften the shock. It is important to pack consistently from jump to jump. It is also important to utilize the same body position with the same speed if you want repetitive openings. The shoulders should level to the horizon, with the body rotating from flat to vertical, through an axis defined by the shoulders, during deployment. This allows for airflow over the back to sweep away any burble, and it positions the jumper, sitting into the saddle of the harness. Use your arms to take some of the opening load by grabbing the risers with your hands during inflation. This will make you ready to take command of your canopy sooner. Be careful not to get your fingers between the risers; they bite. Never look over your shoulder to clear a burble. Look straight up over your head and keep your shoulders level. Uneven shoulders result in uneven line deployment. Looking over your shoulder usually causes you to drop a shoulder, making your body into a propeller. While your body might not start to rotate, the air above you does, and it spins your bag, causing line twists.
In conclusion, I would like to mention the new trend in D-bags, which is to reduce or eliminate the stows. I have seen some that look like they might be OK, and I have seen some that make me run away. The most telling comment I have heard about them is that they don’t work so well on tandems. If you understand all I have said previously, then you know why.



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