Impinging film cooling as an efficient design of the cooling structure can be used in the combustor of high-performance aero-engines. In this work, experiments were implemented to investigate the overall cooling effectiveness of the F-type impinging-film structure concerning various geometric parameters and flowing factors. Effects of blowing ratio M\documentclass[12pt]{minimal}
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\begin{document}$$M$$\end{document}, jet-hole diameter d\documentclass[12pt]{minimal}
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\begin{document}$$d$$\end{document}, jet-to plate pitch z\documentclass[12pt]{minimal}
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\begin{document}$$z$$\end{document}, and jet holes spacing y\documentclass[12pt]{minimal}
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\begin{document}$$y$$\end{document} on the overall cooling effectiveness are investigated. Nine configurations with different non-dimensional impinging height Zn\documentclass[12pt]{minimal}
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\begin{document}$${Z}_{n}$$\end{document} (1.5 ≤ Zn\documentclass[12pt]{minimal}
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\begin{document}$${Z}_{n}$$\end{document}≤3.2), non-dimensional jet hole spacing Yn\documentclass[12pt]{minimal}
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\begin{document}$${Y}_{n}$$\end{document} (1.96 ≤ Yn\documentclass[12pt]{minimal}
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\begin{document}$${Y}_{n}$$\end{document}≤3.5), and jet hole diameter d\documentclass[12pt]{minimal}
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\begin{document}$$d$$\end{document} (d=1,1.2,1.6mm\documentclass[12pt]{minimal}
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\begin{document}$$d=\mathrm{1,1.2,1.6}mm$$\end{document}) are studied. Experiment results show that the overall cooling effectiveness η\documentclass[12pt]{minimal}
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\begin{document}$$\eta$$\end{document} increases with the increase of blowing ratios M\documentclass[12pt]{minimal}
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\begin{document}$$M$$\end{document}, and this tendency becomes weaker as the blowing ratio M\documentclass[12pt]{minimal}
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\begin{document}$$M$$\end{document} exceeds 1.31. The non-dimensional impinging height Zn\documentclass[12pt]{minimal}
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\begin{document}$${Z}_{n}$$\end{document}=1.5 makes a high cooling performance at all blowing ratios M\documentclass[12pt]{minimal}
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\begin{document}$$M$$\end{document}. The area-averaged cooling effectiveness of Zn\documentclass[12pt]{minimal}
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\begin{document}$${Z}_{n}$$\end{document}=1.5 is 2.1% higher than that of Zn\documentclass[12pt]{minimal}
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\begin{document}$${Z}_{n}$$\end{document}=2.4 and is 3.2% higher than that of Zn\documentclass[12pt]{minimal}
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\begin{document}$${Z}_{n}$$\end{document}=3.2 at M\documentclass[12pt]{minimal}
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\begin{document}$$M$$\end{document}=1.31. The cooling effectiveness of Yn\documentclass[12pt]{minimal}
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\begin{document}$${Y}_{n}$$\end{document} =1.96 increases by 2% to 5% when compared to Yn\documentclass[12pt]{minimal}
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\begin{document}$${Y}_{n}$$\end{document} =2.56 and Yn\documentclass[12pt]{minimal}
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\begin{document}$${Y}_{n}$$\end{document} =3.5. When the blowing ratio increases, the cooling effects of Yn\documentclass[12pt]{minimal}
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\begin{document}$${Y}_{n}$$\end{document}=1.96 and Yn\documentclass[12pt]{minimal}
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\begin{document}$${Y}_{n}$$\end{document}=2.56 are almost identical. At the same open percentage and cold air flow rate, the cooling effectiveness of d=1.2mm\documentclass[12pt]{minimal}
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\begin{document}$$d=1.2mm$$\end{document} is 0.8% ~ 2.5% higher than that of d=1mm\documentclass[12pt]{minimal}
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\begin{document}$$d=1mm$$\end{document} and is 2.3% ~ 6% higher than that of d=1.6mm\documentclass[12pt]{minimal}
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\begin{document}$$d=1.6mm$$\end{document}. Finally, using the experimental data, empirical correlations were proposed to fit the overall cooling effectiveness based on the flow and geometrical parameters.