The efficient conditions guaranteeing the existence of positive T-periodic solution to the p-Laplacian–Liénard equation
(ϕp(x′(t)))′+f(x(t))x′(t)+α1(t)g(x(t))=α2(t)xμ(t),\documentclass[12pt]{minimal}
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\begin{document}$$\bigl(\phi _{p}\bigl(x'(t)\bigr) \bigr)'+f \bigl(x(t)\bigr)x'(t)+\alpha _{1}(t)g\bigl(x(t)\bigr)= \frac{ \alpha _{2}(t)}{x^{\mu }(t)}, $$\end{document} are established in this paper. Here ϕp(s)=|s|p−2s\documentclass[12pt]{minimal}
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\begin{document}$\phi _{p}(s)=|s|^{p-2}s$\end{document}, p>1\documentclass[12pt]{minimal}
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\begin{document}$p>1$\end{document}, α1,α2∈L([0,T],R)\documentclass[12pt]{minimal}
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\begin{document}$\alpha _{1},\alpha _{2}\in L([0,T],{R}) $\end{document}, f∈C(R+,R)\documentclass[12pt]{minimal}
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\begin{document}$f\in C({R}_{+},{R})$\end{document} (R+\documentclass[12pt]{minimal}
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\begin{document}${R} _{+}$\end{document} stands for positive real numbers) with a singularity at x=0\documentclass[12pt]{minimal}
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\begin{document}$x=0$\end{document}, g(x)\documentclass[12pt]{minimal}
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\begin{document}$g(x)$\end{document} is continuous on (0;+∞)\documentclass[12pt]{minimal}
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\begin{document}$(0;+\infty )$\end{document}, μ is a constant with μ>0\documentclass[12pt]{minimal}
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\begin{document}$\mu >0$\end{document}, the signs of α1\documentclass[12pt]{minimal}
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\begin{document}$\alpha _{1}$\end{document} and α2\documentclass[12pt]{minimal}
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\begin{document}$\alpha _{2} $\end{document} are allowed to change. The approach is based on the continuation theorem for p-Laplacian-like nonlinear systems obtained by Manásevich and Mawhin in (J. Differ. Equ. 145:367–393, 1998).
