If you've been following this thread, then you know that some people have misinterpreted part of NIST's NCSTAR 1-9 Volume 2 section 12.5.3 as a claim that WTC 7's north wall descended at
exactly 1g for 2.25 seconds.
You also know that the nonlinear model described in NIST's section 12.5.3 describes
- average acceleration of almost 1g for those 2.25 seconds
- instantaneous acceleration of 1g or greater for almost 1 second out of those 2.25 seconds
In the acceleration graph below, which uses
femr2's time scale, the 2.25 seconds in question run from about 12.65 to 14.9 seconds, and the interval of acceleration at 1g or greater runs from about 13.56 to 14.53 seconds.
NIST's section 12.5.3 never states the average acceleration given by its model for the 2.25s interval in question. Although it's easy to calculate, and several recent posts have suggested that its value might contradict parts of NIST's section 12.5.3, I don't think anyone has yet done the calculation.
After I correct an error in one of my responses to
femr2, I will perform the calculation, quote the relevant passage
of from
NIST section 12.5.3, and draw a few conclusions.
My error referred to NIST's Figure 12-77, which
femr2 has extracted for us:
The red line is NIST's linear approximation to part of NIST's nonlinear approximation.
No, the red line is NIST's linear approximation to NIST's data points for Stage 2. The purpose of that red line was to provide an empirical test (sanity check) of NIST's model during Stage 2, whose formula for velocity is shown in the boxed legend at the upper left. The formula for the red line is shown in the boxed legend at the bottom right.
(The rest of the paragraph in which my error appeared remains correct.)
Here's what NIST's section 12.5.3 says about Figures 12-76 and 12-77:
NIST said:
Figure 12–76 presents a plot of the downward displacement data shown as solid circles. A curve fit is also plotted with these data as a solid line. A function of the form z(t) = A{1 – exp[–(t/λ)k]} was selected because it is flexible and well-behaved, and because it satisfies the initial conditions of zero displacement, zero velocity, and zero acceleration. The constants A, λ, and k were determined using least squares fitting. The fitted displacement function was differentiated to estimate the downward velocity as a function of time, shown as a solid curve in Figure 12–77. Velocity data points (solid circles) were also determined from the displacement data using a central difference approximation. The slope of the velocity curve is approximately constant between about 1.75 s and 4.0 s. To estimate the downward acceleration during this stage, a straight line was fit to the open-circled velocity data points using linear regression (shown as a straight line in Figure 12–77). The slope of the straight line, which represents a constant acceleration, was found to be 32.2 ft/s2 (with a coefficient of regression R2 = 0.991), equivalent to the acceleration of gravity g. Note that this line closely matches the velocity curve between about 1.75 s and 4.0 s.
To review: the velocity curve (black curve in Figure 12-77) comes from NIST's nonlinear model, which was obtained by least squares fitting over the entire interval from 0 to 5.4 seconds on NIST's time scale (which corresponds to about 10.9 to 16.3 seconds on
femr2's time scale). The straight red line in Figure 12-77 comes from least squares fitting of a linear model to NIST's data points for the Stage 2 interval from 1.75 to 4.0 seconds on NIST's time scale (which corresponds to about 12.65 to 14.9 seconds on
femr2's time scale).
How closely does the red line match the velocity curve between 1.75 s and 4.0 s? The red line corresponds to a constant acceleration of about 32.2 ft/s
2. The velocity curve corresponds to an average acceleration of about 30.24 ft/s
2 during Stage 2. So NIST was saying that 32.2 is close to 30.24.
The value of 30.24 ft/s
2 comes from NIST's nonlinear model, as displayed by the black lines in Figures 12-76 and 12-77. By the fundamental theorem of calculus, integrating NIST's nonlinear model for acceleration over the interval from 1.75 to 4.0 seconds is equivalent to subtracting the value given by NIST's nonlinear model for velocity at 1.75s from the value given by that model at 4.0s. That tells us that, according to NIST's nonlinear model, the change in velocity was about 68.0 ft/s during that interval. Dividing by the 2.25s duration of the interval gives us the average acceleration: about 30.24 ft/s
2.
With better data, as has been provided by
femr2, we can do a better job of estimating the average acceleration during NIST's Stage 2. Fitting a second degree polynomial to
femr2's vertical displacement data for the NW corner of WTC 7 from 12.65s to 14.9s, and differentiating twice, I got 33.34 ft/s
2, which is slightly higher than NIST's estimate of 32.2 ft/s
2 for the entire north wall.
Some people might wonder how the average acceleration of the NW corner could have been greater than 1g during NIST's stage 2. From physics, we know that when a moderately rigid object is undergoing some rotation as it falls, the largest differences between the acceleration of its center of mass and the acceleration of a particular point on the object are likely to occur at the object's most extreme points. The NW corner is an extreme point of the north wall.
Before we leave the subject of
femr2's data, let's calculate the average acceleration during Stage 2 for a
version of NIST's nonlinear model whose parameters have been recalculated using femr2's data for the NW corner. We would expect that recalculated model to provide a better match for the acceleration calculated from
femr2's data, and it does: applying the fundamental theorem of calculus as before, the change in velocity during Stage 2 is about 76.65 ft/s, and the average acceleration is about 34.1 ft/s
2.
In conclusion, NIST's linear regression (the red line in Figure 12-77) served as a sanity check on its nonlinear model (the black curve in Figure 12-77). NIST found the agreement between its linear regression and its nonlinear model to be close but not exact. Using
femr2's data for the NW corner to estimate the average acceleration during Stage 2 and to recalculate the parameters of NIST's nonlinear model improves the agreement between NIST's nonlinear model and observation.