Shernren,
I am quite frankly shocked that anyone would call a theory a fraud on the basis of pulsar data. (I don't know whether you personally like the word "fraud", but be it baseless garbage or whatever the word is, the outright dismissal is the concept.)
Pulsar data has been measured for how many years? 2,000 or so? Well, no. Less than a century. And Bridgman kills Setterfield on his data set for measuring light speed? Please.
Pulsar data and the aging of these stars is "theory."
Setterfield's work is "theory."
That his assumptions don't fit Bridgmans, I understand that. What that means is that there isn't a "rule out" diagnosis possible for Setterfield, at least not the way Bridgman did it.
This is tiresome. It is nothing new. Been there. Done that.
You know what is tiresome? The way you raise your objections shows that you have made absolutely no effort to try to understand what Bridgman was trying to do. We have tried to understand your source; the least we ask is the courtesy for you to try to understand ours. I have even offered (twice now) to offer as much mathematical help as you need to personally verify or disprove the equations involved.
Anyways, here's the Cliff Notes' version of the problem with the pulsars.
The graph on page 12 shows how a periodic phenomenon will appear to speed up to a distant observer, with the mathematics of it covered via calculus in pp. 8-11. As the speed of light decreases throughout the whole universe at the same time, the speed of light when the pulsar (or, in general, any periodic emitter) emits light is much higher than the speed of light when we observe that light. Crudely speaking, this "mismatch" causes the periodic phenomenon to appear to speed up to us, i.e. its period will decrease. (If the speed of light was increasing between emission and reception, the period would increase instead.)
By using the exact functions Setterfield provides, it is possible to determine exactly how much speed-up each pulsar will experience. Assuming that distance estimates to the pulsars are accurate (an assumption Setterfield himself uses), it is possible to figure out how much the "mismatch" between speed at emission and speed at reception will be different. (Note that what we receive now was emitted many thousands of years ago when in cDK lightspeed was heavily changing, therefore the data
is pertinent - even if it is observed in the present when the speed of light doesn't appear to change to us in our time.) It is then possible to plot how much "mismatch"-speeding up each pulsar should experience vs its distance from us. This is graphed by the lines; they are dotted because the period is decreasing (if something goes faster, it takes less time), meaning that the quantity dP/dt (rate of change of P) is negative.
We have reliable data on how the periods of pulsars have been changing over some time, and hence we can plot actual data onto that theoretical plot. If Setterfield's model is right, we should expect the data points to fall neatly on the curve, showing that there is indeed a large mismatch between pulsar emission lightspeed and our reception lightspeed. Instead, the data points cluster around zero, showing in turn
zero mismatch (other than dynamical spin-down inherent to the pulsars which is orders of magnitude smaller than cDK change).
And now, having explained the relevance of the data, here it is again:
Terrible things happen when you take a physical theory too seriously ...