We consider delay differential equations of the form \( y^{\prime }(t)=-ay(t)+bf(y(t-1)) \) with positive parameters a, b and a unimodal \(f:[0,\infty )\rightarrow [0,1]\) . It is assumed that the nonlinear f is close to a function \(g:[0,\infty )\rightarrow [0,1]\) with \(g(\xi )=0\) for all \(\xi >1\) . The fact \(g(\xi )=0\) for all \(\xi >1\) allows to construct stable periodic orbits for the equation \(x^{\prime }(t)=-cx(t)+dg(x(t-1))\) with some parameters \(d>c>0\) . Then it is shown that the equation \( y^{\prime }(t)=-ay(t)+bf(y(t-1)) \) also has a stable periodic orbit provided a, b, f are sufficiently close to c, d, g in a certain sense. The examples include \(f(\xi )=\frac{\xi ^k}{1+\xi ^n}\) for parameters \(k>0\) and \(n>0\) together with the discontinuous \(g(\xi )=\xi ^k\) for \(\xi \in [0,1)\) , and \(g(\xi )=0\) for \(\xi >1\) . The case \(k=1\) is the famous Mackey–Glass equation, the case \(k>1\) appears in population models with Allee effect, and the case \(k\in (0,1)\) arises in some economic growth models. The obtained stable periodic orbits may have complicated structures.