Multiply the first equation by $x \cdot k(x)$ and the second by $v$, then sum both of them. You obtain $$ x k(x) x'+vv'=-b(v)v^2. $$ Let $V(x)$ such that $V'(x)=x k(x)$, then $$ \frac{d}{dt}\left(\frac{v^2}{2}+V(x)\right)=-b(v)2^2\leq 0 $$ Consider the energy function $E(x,v)=\frac{v^2}{2}+V(x)$. Since it is not increasing in time, $$ \frac{v^2}{2}+V(x)\leq E(0). $$ Now, by physical grounds, $k(x)\geq 0$, then $V(x)$ is bounded from below; we can assume $V(x)\geq 0$ without loss of generality. Therefore $$ |v(t)|\leq \sqrt{2E(0)}. $$ If $k(x)\geq c>0$ (the spring does not become soft for $x\to\infty$), from $V(x)\leq E(0)$ you can also deduce $|x|\leq c_1$. Then the bound $|v'(t)|\leq c_2$ follows from the second differential equation.