Bond dissociation under steadily rising force occurs most frequently at a t
ime governed by the rate of loading (Evans and Ritchie, 1997 Biophys. J. 72
:1541-1555). Multiplied by the loading rate, the breakage time specifies th
e force for most frequent failure (called bond strength) that obeys the sam
e dependence on loading rate. The spectrum of bond strength versus log(load
ing rate) provides an image of the energy landscape traversed in the course
of unbonding. However, when a weak bond is connected to very compliant ele
ments like long polymers, the load applied to the bond does not rise steadi
ly under constant pulling speed, Because of nonsteady loading, the most fre
quent breakage force can differ significantly from that of a bond loaded at
constant rate through stiff linkages. Using generic models for wormlike an
d freely jointed chains, we have analyzed the kinetic process of failure fo
r a bond loaded by pulling the polymer linkages at constant speed. We find
that when linked by either type of polymer chain, a bond is likely to fail
at lower force under steady separation than through stiff linkages. Quite u
nexpectedly, a discontinuous jump can occur in bond strength at slow separa
tion speed in the case of long polymer linkages. We demonstrate that the pr
edictions of strength versus log(loading rate) can rationalize conflicting
results obtained recently for unfolding Ig domains along muscle titin with
different force techniques.