EMENDATIONS
In the year
that "Hear No Evil" has been on the web,
numerous individuals have been kind enough to offer suggestions
to improve the accuracy of the analysis. Two points require
significant emendation as discussed below.
Shock
Wave Arrival Time. -
The first
correction concerns the theory by Luis Alvarez that the blur in
the Zapruder film at frame 313 could have been caused by the
shock wave of a gunshot impinging on the camera body. The blur
analysis of the film was based on the premise that Zapruder would
have been startled by the sound of a gunshot, his reaction
causing a sudden angular movement of the camera, which would then
be detectable as blur. The problem is that the strongest angular
motion detectable in the Zapruder film is at frame 313,
coincident with the impact of the fatal bullet. The sound of a
gunshot fired from the sniper's nest in the Book Depository and
striking JFK at frames 312-313 will not arrive at Zapruder's
position until about frame 315. Likewise, the shockwave from a
bullet on a path from the book depository to JFK will not arrive
at Zapruder's position until after frame 313 is exposed. However,
the calculations provided in HNE in support of this assertion
were incorrect.
The shock wave
arrives at Zapruder's position ahead of the sound of the muzzle
blast because the sound wave must travel a distance of 270 ft on
a direct path to reach Zapruder, and at the speed of sound (1123
fps at 65F) this time is 240 msec. The shock wave emanates from
the nose of the bullet and although the shockwave must travel a
longer path to reach Zapruder, it travels at twice the speed of
sound during the longer leg of its approach. As the shock wave is
shed from the bullet it quickly returns to its natural speed in
air, which is the speed of sound, for its last leg towards
Zapruder. I erroneously assumed that the front of the shock wave
reaching Zapruder would emanate from the point on the bullet's
path closest to Zapruder, which would have been just before
striking JFK. However, Physicist Paul Hoch has pointed out that
because the angle of approach towards Zapruder is increasing, the
speed of approach towards Zapruder is decreasing, and becomes
less than the speed of sound at some point upstream from the
target. It is from there that the shock wave front will emanate
towards Zapruder. By calculating the arrival of the shock wave
from a series of points along the bullets path at 10 ft
intervals, I find that Hoch is correct. The shock wave, which
reaches Zapruder, emanates from a point approximately 210 ft
downstream from the muzzle.
In redoing
these calculations a second error was discovered. A witness for
the HSCA estimated that the impact velocity of the fatal bullet
would have been around 1600 fps, and I employed that value in my
earlier calculations. However, Alfred Olivier provided more
precise values of the bullets velocity in his testimony to
the Warren Commission. The muzzle velocity of Oswald's rifle was
2160 fps. The bullet's velocity at 60 yds (180 ft) was 1904 fps.
The bullet slows down due to air resistance; however, at the rate
of slowing measured by Olivier the bullet's velocity at 265 ft
would have been significantly greater than the HSCA's estimate of
1600fps. This was confirmed by checking ballistic tables for
similar bullets (the 6.5 mm Carcano bullet weighed 160 grains).
For example, a Winchester .30 caliber 170-grain bullet with an MV
of 2200 fps has a velocity of 1900 fps at 100 yds (300 ft). A
Remington .35 caliber, 200-grain bullet at MV 2080 fps, has a
velocity at 300 ft of 1800 fps. A Remington .27 cal 120-grain
bullet with the same MV of 2080 fps also has the same velocity at
300 ft of 1800 fps. Subsequently I found the value of 1800 fps
adopted by Luis Alvarez in his studies of the ballistics in this
case (Alvarez 1976, Am. J. Phys. p. 821) and this value, if not
exact, is at least coherent with the measurements of Olivier.
The table
below shows the shock wave arrival times from different points in
the trajectory and the values used to obtain the times. D1 is the
distance from the muzzle in feet; D2 is the distance from the end
point in D1 to Zapruder. V1 is the muzzle velocity (in fps); V2
is the velocity at the end point of D1. Vm is the mean velocity
for D1, which is V1+V2/2. T1 is the time for the bullet to travel
D1, which is D1/Vm. T2 is the time for the shock wave to travel
from the end point of D1 to Zapruder. T1+T2 is the time at which
the shock wave arrives at Zapruder after trigger time (all times
in milliseconds).
D1
D2 V1
V2 Vm T1
T2 T1+T2
180
109 2160 1904 2032
89 97 186
msec
190
102 2160 1889 2025
94 91 185
msec
200
93 2160 1875 2018
99 85 184
msec
210
88 2160 1862 2011
104 78 182
msec
220
83 2160 1852 2006
110 74 184
msec
From this
table it can be seen that the shock wave emanates from a point
approx. 210 ft downstream from the muzzle and reaches Zapruder
182 msec after trigger time.
The mean
velocity of the bullet between the sixth floor and JFK would have
been (2160+1800)/2 = 1980 fps. At this speed the impact time of
the bullet would be at 265/1980 = 134 msec after trigger time.
Therefore, the shock wave arrives at Zapruder 48 msec after
impact time. For the reasons explained in HNE, impact time was
approx. 15 msec before the exposure of Z-313 begins. Because the
exposure time is approx. 27 msec, Z-313 exposure ends at 42 msec
after impact and 6 msec before the shock wave arrives. Thus, even
if the shock wave were supposed to be strong enough to cause a
jerky motion in Zapruder's camera body, it does not arrive in
time to cause the angular motion evident at Z-313.
Position
of Car-8. -
In the 20th
frame of the third sequence of Robert Hughes' film of the
President's motorcade, H.B. McLain's motorcycle is seen at the
intersection of Houston and Main Streets. McLain is the only
motorcycle patrolman that could have been at the acoustically
predicted locations to capture the sounds of the assassination
gunfire. In HNE it was estimated that H20 correlated to a time
approx. 6-7 sec before the first shot. This estimate relied on
two values; one was an estimate of the average speed of the
eighth car in the motorcade of approx. 7 mph. The other was the
distance of Car-8 between where it is seen in H20 and where it is
seen in Zapruder frame 220. In HNE I estimated this distance to
be 88 ft.
The position
of Car-8 in the Zapruder film can be determined by a line of
sight from Zapruder's position through a small oak tree in Dealey
Plaza, both of which can be fixed accurately, and which line
intercepts the front bumper of Car-8 at frame 220. Michael Russ
has suggested that a similar line of sight could be applied to
the Hughes film to fix the earlier position of Car-8. Such an
analysis is problematic because, unlike the Zapruder case,
Hughes' position is not known precisely. In a photograph taken by
Charles Bronson just as the President's motorcade arrived at the
intersection one can see the crowd of people where Hughes must be
standing. Hughes has to be standing among this crowd because were
he standing further back he would not have had an unobstructed
view of the motorcade as seen in the film. As the motorcade
approached, Hughes' aimed his camera east down Main Street. His
line of sight indicates that he was standing almost exactly in
line with the road stripe separating the eastbound lanes of
traffic, or slightly to the north of this line. As he panned to
his left following the motorcade he eventually pointed his camera
north on Houston Street. From this line of sight it can be seen
that he was standing almost exactly in the middle of the western
most lane of traffic, or judging by the line of grease spots,
slightly to the west. The intersection of these two lines gives
us a fair approximation of Hughes' position. Assuming the traffic
lanes were 9 ft wide, this position can be defined as 8 ft south
of the center line of Main Street and 14 ft west of the center
line of Houston Street. We have to assume this width because the
lines have been repainted since 1963. In 1963 Houston was a two
way street with four lanes of traffic. Today it is a one-way
street with three lanes of traffic. By north and south I am
referring to the general orientation, as the streets of Dallas
are not laid out in the cardinal compass directions. I have
plotted Hughes' position on a topographic map of Dealey Plaza. I
have also plotted a line of sight from Hughes to the corner of
the Records Building because Car-8 lies on this line of sight.
Also, the left front corner of Car-9 just intercepts this line.
From Hughes' viewpoint the view of Car-8 was partially blocked by
Car-9 as shown in the juxtaposition on the map. The Hughes photo
shows an offset in that the left side of Car-8 aligned with the
midstripe on Houston Street, whereas Car-9 was about 2-3 ft to
the east of the line. As a further corroboration for the plotted
location I have drawn in the crosswalk stripe, which can be seen
about half a car-length behind Car-9 in H20. My error in the
corresponding map in HNE was to misplace this stripe too far
south (there were actually 3 stripes). The correct position of
the stripe is in line with the first window of the Court House.
With this corrected position for Car-8 the distance from its
position in Z-220 (front bumper to front bumper) is 73 ft, about
a car-length further north than its position plotted earlier (the
plot provided is diagrammatic, the actual measurement was made on
the published HSCA survey map with proportional cut-outs
representing the cars which were 15x7 ft in dimension).
In order to
correlate H20 to the Zapruder film we need an estimate of the
speed of Car-8. In the Zapruder film Car-8 has a velocity of 8.5
mph. However, one cannot apply this rate of speed to the entire
interval between H20 and Z-220 because the speed of the motorcade
was known to vary. For example, Car-5 can be seen rounding the
corner in the Zapruder film at about this same time and it is
traveling at only 5.5 mph. This indicates that the cars would
slow down for the turns and then speed up in the straight-aways.
This would cause an accordion effect in the motorcade with the
cars always speeding up or slowing down as the drivers reacted to
the cars ahead. Because Car-8 seen in the Zapruder film is in the
middle of the straightaway it was most likely at or close to
maximum speed. Therefore the most likely average speed for Car-8
between Z-220 and H-20 would have been around 6-8 mph. This
corresponds to a speed of 8.8 to 11.7 fps. Therefore, the time
lapse to cover the distance of 73 ft between Z-220 and H20 would
be in a range from 6.2 to 8.3 sec. The first shot correlated to
Zapruder frame 175, which is 2.4 sec prior to Z-220 (at 18.3
frames/sec). Therefore, from his position at the intersection of
Houston and Main, McLain had approx. 3.8 to 5.9 sec to reach the
first acoustically identified position 180 ft away. The 5.9 sec
estimate requires McLain to travel at an average speed of 20.8
mph. The 3.8 sec timeframe would require a speed of 32 mph. A
middle value of 5 sec requires a speed of 25 mph.
Another film
gives support to the inferred speeds. In H20, McLain's motorcycle
is close to Car-10 at the intersection of Houston and Main. When
Car-10 rounded the intersection at Elm and Houston, Malcolm
Couch, a newsreel photographer in Car-10, aimed his camera down
Elm Street and filmed McLain approx. 200 ft away to the west.
This means that in the time that it took Car-10 to travel 200 ft
from Main to Elm, McLain had traveled 400 ft. Therefore his
average speed during the interval has to have been twice whatever
Car-10 was doing. In this newsreel Cars-8, 9 and 10 are only
about a car length apart, just as they were in the Hughes film.
If the cars averaged 7 mph on Houston Street, then McLain had to
average 14 mph during the same interval. However, this speed has
to be apportioned in accordance with the acoustical data which
indicates a faster speed prior to the shots and then an idle
speed after the shots. Seconds before the first sound
acoustically identified as a gunshot occurs, the motorcycle motor
noise diminished by 75%, indicating that the driver let off the
accelerator, presumably in anticipation of making the turn around
Elm and Houston. For the next 30 sec the motor continued at idle.
The acoustical data require a speed of 11-12 mph during the
shooting when the motorcycle would have to be rounding the
corner. Thus, a required speed of 20-25 mph for McLain on Houston
Street is in accord with both the acoustical and the filmed
evidence. It should be understood that these values are soft
values, which is to say, they are inferences from observed data,
not actual measurements, and therefore do not prove that McLain
was in the right position to record the shots, only that he
reasonably could have been.
Donald
Thomas
January
2003

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