S
Seiji Yoshida
Researcher at Japan Aerospace Exploration Agency
Publications - 16
Citations - 149
Seiji Yoshida is an academic researcher from Japan Aerospace Exploration Agency. The author has contributed to research in topics: Combustor & Combustion. The author has an hindex of 7, co-authored 14 publications receiving 109 citations.
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Combined effect of spatial and temporal variations of equivalence ratio on combustion instability in a low-swirl combustor
TL;DR: In this paper, the combined effect of spatial and temporal variations of fuel-air mixture on self-excited combustion instabilities in a gas-turbine model combustor (∼60kW) with a low-swirl injector is reported.
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Large-Eddy Simulation of High-Frequency Combustion Instability in a Single-Element Atmospheric Combustor
TL;DR: In this paper, a large-eddy simulation is performed to simulate high-frequency combustion instability in a single-element atmospheric combustor, and the coupling mechanism between the flame and acoustic mode is explored based on the largeeddy simulation results.
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Detection of frequency-mode-shift during thermoacoustic combustion oscillations in a staged aircraft engine model combustor
TL;DR: In this paper, the authors used time series analysis based on symbolic dynamics to detect a precursor of frequency-mode shift during thermoacoustic combustion oscillations in a staged aircraft engine model combustor.
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Dynamic behavior of intermittent combustion oscillations in a model rocket engine combustor
TL;DR: In this paper, the dynamic behavior of intermittent combustion oscillations by time series analysis in terms of nonlinear forecasting, symbolic dynamics, and statistical complexity, including the detection of the change in dynamical state based on symbolic dynamics and graph networks.
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Intense Tangential Pressure Oscillations Inside a Cylindrical Chamber
TL;DR: In this article, a coaxial injector is installed offcenter on the closed side of a cylindrical chamber to generate the tangential pressure oscillations due to oscillatory combustion, and the amplitude of the positive halfwave (zero to positive peak) of the pressure oscillation is larger than that of the negative half-wave (negative peak to zero).