Non-renormalizable field theories contain non-renormlizable operators whose couplings have negative mass dimension (for example, Fermi coupling in the Fermi theory of weak interaction). These couplings provide an energy scale $\Lambda$ built into the theory, and it is said that the predictions above energy $E\geq \Lambda$, is not reliable.
How does one understand whether the predictions of a nonrenormalizable theory, below $\Lambda$ are reliable but bound to fail above $\Lambda$?
Consider a renormalizable theory such as the Standard model. There is no built-in length scale. Therefore, if its predictions are tested at energy $E=E_1$, can we not claim that it's predictions, will be perfectly reliable to arbitrarily high energies (for example, $E=10^{16}\times E_1$), if there is no new physics that enter in between.
Such a claim may be (or must be?) false for a nonrenormalizable theory. Isn't it?