In Ohm's Law, V and I are variables, but R is a parameter.
Ohm showed that for many useful situations, R is a constant over a wide range of the two variables.
Ohm's Law (when valid) is more than a definition of the ratio R, it is an explicit statement that R is constant (for a given component).
Ohm's Law, and other uses of the word "ohm":
Meanwhile, the actual Ohm's Law (for linear ohmic materials only) has some interesting implications, only valid for linear ohmic materials.
To calculate the resistance of a long wire or similar geometry, with constant cross-section area, one can treat it as a series of short wires in series, or a series of long skinny wires in parallel.
This results in the well known formula
R = {rho} x l / A ,
where {rho} is another constant (the resistivity of the material, usually given in ohm-cm), l is the length of the wire, and A is the cross-sectional area.
Again, this only works for a linear ohmic material.
The reversal of slope in a tunnel diode is often called a negative resistance, but that is not an ohmic device.
It is straightforward to define the "ohm" unit from Ohm's Law as the ratio of volts per ampere, and use that unit for the derivative dV/dI, but that is not Ohm's Law.
As an analogy, one defines "efficiency" as the ratio of output power divided by input power.
Obviously, efficiency depends on all the variables, such as shaft rpm or power level for a motor.
It would be foolish to assume that efficiency of a practical device is constant over the useful range of the device.