Hello again, I decided I couldn't do a good job on your lever ratio post; but, maybe I can be of more assistance this time around. As I stated above, the amount of resisting force is dependent upon how far you compress the cylinder. To start the initial amount of force is dependent upon how high you pressurize the cylinder and will increase as you reduce the volume in the cylinder by compressing it.
For a start, the force at any given point is dependent on the area of the cylinder bore x the pressure in the cylinder at that point.
For example, you state that you have an 80 mm bore which results in a piston area of 80^2 x pi() / 4 = 5027 mm^2 of area, for your first case of pressurizing the cylinder to 1 Bar then the resulting initial resisting force of the cylinder will = 503 N; and, for 1.5 Bar that force = 1.5/1 x 503 = 754 N.
Now that we that using a simple P1V1 = P2V2 relationship, which can be stated as: P1 x A x L1 = P2 x A x L2 where P1 is the initial pressure from above; A is the Area of the Piston = 5027 mm^2; L1 is initial distance at full rod extension = 172 mm; and P2 is the resulting pressure at L2 = L1 - S (Stroke distance)
By multiplying P1 x A = F1 (force at full rod extension) and P2 x A = F2 ( force at L1 - S), which leaves F1 x L1 = F2 X (L1- S) or better for your purpose:
F2 = (P1 x A) x L1 / (L1 - S).
Now for any initial cylinder Pressure, you can determine F2 at each selected Stroke length.
From a scientific point there are more sophisticated formulas based upon the basic gas laws; but, this calculation will give you a reasonably accurate resisting force of the cylinder at each initial cylinder pressure and stoke length combination. PS The force increase is linear with the stroke increase, if the stroke is slow enough to allow the cylinder wall to cool the gas during the stroke; if not, the above formula becomes F2 = [(P x A) / (L1- S)] x (T2 / T1) where T2 and T1 are given in °R and T2 must be calculated using the classic gas equation for compression heating based upon T2 = T1 x P2/P1 and the properties of the gas.