This work is concerned with the stabilization of hyperbolic systems by a nonlinear
feedback which can be localized on a part of the boundary or locally distributed. We show that general weighted integral inequalities together with
convexity arguments allow us to produce
a general semi-explicit formula which leads to decay rates of the energy in terms of the behavior of the nonlinear
feedback close to the origin.
This formula allows us to unify
for instance the cases where the feedback has a polynomial growth at the origin, with the cases
where it goes exponentially fast to zero at the origin. We also give three other significant examples
of nonpolynomial growth at the origin. Our work completes the work
of [15] and improves the results of
[21] and [22]
(see also [23]
and [10]). We also prove the optimality of our results for the one-dimensional wave equation
with nonlinear boundary dissipation. The key property for obtaining our general energy
decay formula is the understanding between convexity properties of an explicit function
connected to the feedback and the dissipation of energy.