Critical current and flux pinning densities have been determined for a series of practical conductors as a function of uniaxial tensile strain in magnetic fields ranging from 4 T to 19 T. An empirical relation has been found at 4.2 K that accurately describes these data over the entire range of field under both compressive and tensile strain. The pinning force F has been found to obey a scaling law of the form:
![F = [B*_{c2}(\\varepsilon )]^{n} f(b)](/images/tex/8843.gif)
where f(b) is a function only of the reduced magnetic field

, and

is the strain dependent upper-critical field determined from high-field critical-current measurements. This strain scaling law was found to hold for all superconductors examined thus far, including commercial multifilamentary wire, mono-filamentary conductors, CVD tapes, extremely fine-filament conductors, partially-reacted specimens, and "in-situ" cast conductors. For Nb
3Sn,

, for Nb
3Sn with Hf and Ga additions,

, for V
3Ga,

, for Nb
3Ge,

, and for NbTi,

. The importance of this relationship is that, for these conductors at least, it is possible to measure F at one strain and then immediately be able to predict F (and thus J
c) at other strain levels simply by scaling the results by
![[B*_{c2}(\\varepsilon )]^{n}](/images/tex/8851.gif)
. The relation between strain scaling and temperature scaling is discussed as it relates to flux pinning theories.