2022
DOI: 10.1016/j.actaastro.2021.12.027
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Uncertainty analysis and calibration of SST turbulence model for free shear layer in cavity-ramp flow

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Cited by 16 publications
(7 citation statements)
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“…The total variance of quantities of interests obtained from the surrogate model can be decomposed as 16 Dgoodbreak=i=1i=nDigoodbreak+1i<jni=n1Di,jgoodbreak+1i<j<kni=n2Di,j,kgoodbreak+goodbreak+D1,2,,n$$ D=\sum \limits_{i=1}^{i=n}{D}_i+\sum \limits_{1\le i<j\le n}^{i=n-1}{D}_{i,j}+\sum \limits_{1\le i<j<k\le n}^{i=n-2}{D}_{i,j,k}+\dots +{D}_{1,2,\dots, n} $$ lefttruelmatrixDi1,,is=false∑βi1,,isbold-italiccβ2bold-italicψβ2false(bold-italicξfalse),1i<<isn.$$ {\displaystyle \begin{array}{l}\\ {}{D}_{i_1,\dots, {i}_s}=\sum \limits_{\beta \in \left({i}_1,\dots, {i}_s\right)}{\boldsymbol{c}}_{\beta}^2\left\langle {\boldsymbol{\psi}}_{\beta}^2\left(\boldsymbol{\xi} \right)\right\rangle, \kern0.5em 1\le i<\dots <{i}_s\le n.\end{array}} $$ …”
Section: Bayesian Optimization Methods and Uncertainty Quantificationmentioning
confidence: 99%
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“…The total variance of quantities of interests obtained from the surrogate model can be decomposed as 16 Dgoodbreak=i=1i=nDigoodbreak+1i<jni=n1Di,jgoodbreak+1i<j<kni=n2Di,j,kgoodbreak+goodbreak+D1,2,,n$$ D=\sum \limits_{i=1}^{i=n}{D}_i+\sum \limits_{1\le i<j\le n}^{i=n-1}{D}_{i,j}+\sum \limits_{1\le i<j<k\le n}^{i=n-2}{D}_{i,j,k}+\dots +{D}_{1,2,\dots, n} $$ lefttruelmatrixDi1,,is=false∑βi1,,isbold-italiccβ2bold-italicψβ2false(bold-italicξfalse),1i<<isn.$$ {\displaystyle \begin{array}{l}\\ {}{D}_{i_1,\dots, {i}_s}=\sum \limits_{\beta \in \left({i}_1,\dots, {i}_s\right)}{\boldsymbol{c}}_{\beta}^2\left\langle {\boldsymbol{\psi}}_{\beta}^2\left(\boldsymbol{\xi} \right)\right\rangle, \kern0.5em 1\le i<\dots <{i}_s\le n.\end{array}} $$ …”
Section: Bayesian Optimization Methods and Uncertainty Quantificationmentioning
confidence: 99%
“…In this study, it is worth noting that the upper and lower bounds of these parameters were determined based on the ratio between parameters β*false/β1$$ {\beta}^{\ast }/{\beta}_1 $$ and β*false/β2$$ {\beta}^{\ast }/{\beta}_2 $$. This approach resulted in slight differences compared to the upper and lower limits of β1$$ {\beta}_1 $$ and β2$$ {\beta}_2 $$ provided in Reference 16, which could potentially lead to variation in the importance coefficients. The specific differentiation of importance coefficients is described in Section 4.3.…”
Section: Sst Turbulence Modelmentioning
confidence: 99%
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