The Edgewood tests showed that the simulation of Kennedy's back deformed test bullets to an extent comparable with CE 399 and the simulations of Connally's back and wrist deformed the test bullets to a greater extent than CE 399. From these results, they concluded that the bullet, which inflicted wounds on Connally had slowed considerably before striking.
The experimenters had no way of predicting the details of bullet impact upon the bones. So they placed their velocity screens along a straight line extending from the shooter through the target. As a result they failed to obtain data on bullets, which deflected through larger angles during a prolonged grazing collision with a bone.
During a grazing collision the force from the obstacle upon the bullet is perpendicular to the surface of the obstacle at the point of impact. The direction of this force differs from the bullet's direction of motion. As a result the direction of the bullet changes throughout the duration of the grazing collision. They measure the net change in direction by the deflection angle.
By contrast, a penetrating collision produces negligible deflection of the bullet. In this case the penetrating bullet alters the shape of the impacted obstacle so that the direction of the force from the obstacle is opposite the direction of the bullet. So penetration slows the bullet without changing its direction of motion.
These consideration explain how a bone may deflect a bullet without leaving radiological evidence.
Although the force upon the bullet from a grazing collision is less than the force from a penetrating collision, these forces act over widely varying distances. So the change in kinetic energy of the bullet from a grazing collision maybe larger than for a penetrating collision.
Deflection changes the yaw of a bullet without necessarily inducing yawing. When the action of a force from a grazing collision is asymmetrically distributed about the center of gravity of the bullet, the tangential component of this force produces yawing in addition to deflection. For this reason any obstacle that causes yawing also deflects the bullet. However, the converse of the preceding statement is not always true. An obstacle can deflect a bullet and change its yaw without inducing yawing. In this later case the action of the force is symmetrically distributed about the center of gravity.
The above considerations show that the Edgewood data on relatively un deflected bullets transited and exited the simulations with negligible yaw. This result enables testing the yaw explanation of the sizes of Connally's wounds.
To reconstruct the assassination situation as closely as possible both sides of the substances were covered with material and clipped animal skin to duplicate human skin. The average exit velocity was 1,779 feet from the gelatin, 1,798 feet from the first animal meat and 1,772 feet from the second animal meat.
Using the measured entrance and exit speeds with the revised mass, 7.27 X 10-4 slug, of a MC bullet permits calculation of the kinetic energy lost during transit of the simulated target.
| Average entrance speed | Average exit speed | Loss of kinetic energy | Length of wound track | Mean force | Striking area |
| 1904 fps | 1785 fps | 160 ft-lb | 0.45 ft | 354 lb | 0.049 sq-in |
The reported length of 13.5 to 14 centimeters for the wound track in Kennedy's neck is unrepresentative of the distance from the upper back to the throat of a large adult. For this reason, revised computations use 0.6 ft for the length of the wound track.
| Average entrance speed | Mean force | Length of wound track | Loss of kinetic energy | Average exit speed |
| 1904 fps | 354 lb | 0.6 ft | 213 ft-lb | 1743 fps |
The mean force exerted by the target upon the bullet equals the mean yield stress of the target multiplied by the striking area of the bullet. Since changing the length of the wound track changes neither factor, the mean force is unchanged. So the loss of kinetic energy equals this unchanged force multiplied by the revised length of the wound track.
| Average striking speed | Average exit speed | Loss of kinetic energy | Length of wound track | Mean force | Striking area |
| 1929 fps | 1664 fps | 346 ft-lb | 0.85 ft | 407 lb | 0.049 sq-in |
The loss of kinetic energy by the bullet equals the length of the wound track multiplied by the mean force. Since the mean force equals the mean yield stress of the target multiplied by the striking area, the loss of kinetic energy by the bullet is proportional to striking area of the bullet. So when the yaw angle increases the striking area by a factor k the loss of kinetic energy increases by the same factor. This consideration enables calculation of the largest striking area for the bullet to exit the simulated chest.
The bullet at the striking speed of 1929 fps has a kinetic energy of 1352 ft-lb. For a striking area of 0.049 sq-in the bullet lost a kinetic energy of 346 ft-lb. So the loss of kinetic energy by an exiting bullet can increase by a factor k = 1352 ft-lb / 346 ft-lb or 3.91. Taking the striking area of the yawed bullet, 0.049k, as a rectangle gives a wound whose width is 2r or 0.25 inch and length is 0.049k / (2r) or 0.77 inch.
Combining results from Kennedy's simulated back and neck wounds with Connally's simulated back and chest wounds produce a more realistic description. The test bullet exited the simulated neck with a speed of 1743 fps, lost 3 fps while traveling between targets and struck Connally's simulated back with a speed of 1740 fps. Now the available kinetic energy becomes 1100 ft-lb and reduces k to 3.18. So the dimensions of the rectangular wound become 0.25 inch by 0.62 inch.
The medical evidence documents the longest dimension of Connally's back wound as 0.6 inch. So without the additional burdens of transiting the wrist and penetrating the thigh, attributing the length of Connally's back wound to yaw is marginally feasible.
The average striking velocity of the shots was 1,858 feet per second. The average exit velocity was 1,786 feet per second for the 7 out of 10 shots from bone structures which could be measured. These tests demonstrated that Governor Connally's wrist was not struck by a pristine bullet, which is a missile that strikes an object before hitting anything else. This conclusion was based on the following factors: (1) Greater damage was inflicted on the bone structure than that which was suffered by the Governor's wrist; and (2) the bone structure had a smaller entry wound and a larger exit wound which is characteristic of a pristine bullet as distinguished from the Governor's wrist which had a larger wound of entry indicating a bullet which was tumbling with substantial reduction in velocity. In addition, if the bullet found on the Governor's stretcher (Commission Exhibit No. 399) inflicted the wound on the Governor's wrist, then it could not have passed through the Governor's wrist had it been a pristine bullet, for the nose would have been considerably flattened, as was the bullet which struck the bone structure, identified as Commission Exhibit No. 856.
| Striking speed | Exit speed | Loss of kinetic energy | Length of wound track | Mean force | Striking area | Mean stress |
| 1858 fps | 1786 fps | 95.3 ft-lb | 0.2 ft | 477 lb | 0.049 sq-in | 9730 psi |
In a composite situation with the bullet striking a simulation of Kennedy with a speed of 1904 fps, acquiring a yaw, transiting the simulations of Connally's chest and wrist to emerge with negligible speed requires the factor k to be 1100 ft-lb / ( 346 ft-lb + 95.3 ft-lb ) or 2.49. Allowing an additional loss of 20 ft-lb for the bullet to penetrate a simulated thigh gives the bottom line for the yaw explanation of a single bullet event. The factor k becomes 1100 ft-lb / ( 346 ft-lb + 95.3 ft-lb + 20 ft-lb ) or 2.39. The longest dimension of the rectangular wound is 0.47 inch and discredits the yaw explanation of Connally's back wound.
Clearly the above analysis shows the impossibility of attributing the dimensions of Connally's back and wrist wounds to a single bullet with yaw inflicting seven wounds on two victims.
An accounting of kinetic energy shows the infeasibility of wounding by a pristine bullet. The loss of kinetic energy by a pristine bullet in producing the neck, chest, wrist and thigh wounds would be 213 ft-lb + 346 ft-lb + 95.3 ft-lb + 20 ft-lb. These wounds diminish the initial kinetic energy of 1317 ft-lb by 674 ft-lb. So a single bullet event requires means to consume a kinetic energy of 674 ft-lb. Although the earlier considerations show that the yaw angle of a bullet can consume far more than 674 ft-lb, the experimental design excluded grazing collisions that consume considerable kinetic energy while deflecting and possibly yawing the bullet. Without doubt attributing the consumption of 674 ft-lb to yaw is unsupportable, especially when the shapes and positions of Kennedy's back and neck wounds require a considerable deflection of the transiting bullet.
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