The J570 has a total impulse of 973.1 Ns and a maximum thrust of 1142.4 N (not Ns). On a side note, the plural form "Newtons" should IMHO be avoided because of its ambiguous nature in our context.
The J570 has quite a pronounced erosive spike at the beginning of the burn, as can be seen on the thrust curve provided by Aerotech. This is typical for long motors with WL or many other propellants.
Besides the fixed motor parameters (propellant, geometry), there are many variable factors that will likely influence this spike (type of igniter, igniter location, temperature,..).
Due to the transient nature of this spike, the measured thrust curve will be influenced by the nature of the thrust stand (mass, stiffness, dampening). On a motor with a more gradual rise/decline in thrust, this is less of an issue.
An analogy: If you hit a steel door with a hammer, it will sound differently than a wood door hit with the very same hammer. On the other hand, if you just lean against it, you won't notice a difference, unless it is a really flimsy one.
The electronic data acquisition system has also its particular characteristics, but often the electronics are so "fast" (high bandwidth) compared to the motor and thrust stand that its influence is negligible.
Last but not least, the data is post processed on the computer to put it in a more useful format for end use. This typically involves things like noise reduction (low pass filtering) and a final reduction of data points (the original RASP can only handle max. 32 of them). Both of these steps have the potential to smooth away the spike at the beginning, depending how exactly they are performed.
Because you can't know exactly what your average J570 will do really in your rocket, you should be very conservative. In other words, make sure the rocket can structurally handle the peak and that the rocket will still launch safely if it is not present (launch weight, rail length).
Reinhard