\begin{document}$m_{H^{\pm}} \simeq 184~ {\rm GeV}$\end{document} at a \begin{document}$500~ {\rm GeV}$\end{document} \begin{document}$e^+e^-$\end{document} collider, and decreases consistently with the increase of \begin{document}$\tan\beta$\end{document} in the low \begin{document}$\tan\beta$\end{document} region. The peak in the colliding energy distribution of the cross section arises from the resonance of the loop integrals, and it moves towards the low colliding energy with the increase of \begin{document}$m_{H^{\pm}}$\end{document}. We also study the two-loop NLO QCD corrections to both the integrated cross section and the angular distribution of the charged Higgs boson and find that the QCD relative correction is also sensitive to the charged Higgs mass and strongly depends on the final-state phase space. For \begin{document}$\tan\beta = 2$\end{document}, the QCD relative correction at a \begin{document}$500~ {\rm GeV}$\end{document} \begin{document}$e^+e^-$\end{document} collider varies in the range of [-10%, 11%] as \begin{document}$m_{H^{\pm}}$\end{document} increases from 150 to 400 GeV."> QCD corrections to <inline-formula><tex-math id="M1-12">\begin{document}${{{e^+e^-}}{{\rightarrow}}{{H^{\pm}}}{{W^{\mp}}}}$\end{document}</tex-math><alternatives><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="//www.macurncorp.com/hepnp/article/app/id/effe36ad-c1d0-4a57-afcf-a75054a22913/CPC-2020-0215_M1-12.jpg"/><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="//www.macurncorp.com/hepnp/article/app/id/effe36ad-c1d0-4a57-afcf-a75054a22913/CPC-2020-0215_M1-12.png"/></alternatives></inline-formula> in Type-I THDM at electron positron colliders -
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