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Optimal perturbation (Wo=15, Re_δ=530): snapshots in a (z,r)-cross-section
The data are obtained via an in-house Matlab script (developed by Dr. Baofang Song) to compute the non-modal transient growth of disturbances in pulsatile and oscillatory pipe... -
Optimal perturbation (Wo=10, Re_δ=530): snapshots in a (z,r)-cross-section
The data are obtained via an in-house Matlab script (developed by Dr. Baofang Song) to compute the non-modal transient growth of disturbances in pulsatile and oscillatory pipe... -
Optimal perturbation (helical, Re=2000,A=1,Wo=15): u_z profile t=tf
The data are obtained via an in-house Matlab script (developed by Dr. Baofang Song) to compute the non-modal transient growth of disturbances in pulsatile and oscillatory pipe... -
Optimal perturbation (helical, Re=2000,A=1,Wo=15): u_z profile t=t0
The data are obtained via an in-house Matlab script (developed by Dr. Baofang Song) to compute the non-modal transient growth of disturbances in pulsatile and oscillatory pipe... -
Optimal perturbation (classic, Re=2000,A=1,Wo=15): u_z profile t=tf
The data are obtained via an in-house Matlab script (developed by Dr. Baofang Song) to compute the non-modal transient growth of disturbances in pulsatile and oscillatory pipe... -
Optimal perturbation (classic, Re=2000,A=1,Wo=15): u_z profile t=t0
The data are obtained via an in-house Matlab script (developed by Dr. Baofang Song) to compute the non-modal transient growth of disturbances in pulsatile and oscillatory pipe... -
Optimal perturbation (helical, Re=2000,A=1,Wo=15): snapshot axial vorticity t=tf
The data are obtained via an in-house Matlab script (developed by Dr. Baofang Song) to compute the non-modal transient growth of disturbances in pulsatile and oscillatory pipe... -
Optimal perturbation (helical, Re=2000,A=1,Wo=15): snapshot axial vorticity t=t0
The data are obtained via an in-house Matlab script (developed by Dr. Baofang Song) to compute the non-modal transient growth of disturbances in pulsatile and oscillatory pipe... -
Optimal perturbation (classic, Re=2000,A=1,Wo=15): snapshot axial vorticity t=tf
The data are obtained via an in-house Matlab script (developed by Dr. Baofang Song) to compute the non-modal transient growth of disturbances in pulsatile and oscillatory pipe... -
Optimal perturbation (classic, Re=2000,A=1,Wo=15): snapshot axial vorticity t=t0
The data are obtained via an in-house Matlab script (developed by Dr. Baofang Song) to compute the non-modal transient growth of disturbances in pulsatile and oscillatory pipe... -
Optimal perturbation (helical, Re=2000,A=1,Wo=15): snapshot axial velocity t=tf
The data are obtained via an in-house Matlab script (developed by Dr. Baofang Song) to compute the non-modal transient growth of disturbances in pulsatile and oscillatory pipe... -
Optimal perturbation (helical, Re=2000,A=1,Wo=15): snapshot axial velocity t=t0
The data are obtained via an in-house Matlab script (developed by Dr. Baofang Song) to compute the non-modal transient growth of disturbances in pulsatile and oscillatory pipe... -
Optimal perturbation (classic, Re=2000,A=1,Wo=15): snapshot axial velocity t=tf
The data are obtained via an in-house Matlab script (developed by Dr. Baofang Song) to compute the non-modal transient growth of disturbances in pulsatile and oscillatory pipe... -
Optimal perturbation (classic, Re=2000,A=1,Wo=15): snapshot axial velocity t=t0
The data are obtained via an in-house Matlab script (developed by Dr. Baofang Song) to compute the non-modal transient growth of disturbances in pulsatile and oscillatory pipe... -
Optimal perturbation (helical, Re=2000,A=1,Wo=15): Time series of the r-theta...
Laminar flows through pipes driven at steady, pulsatile or oscillatory rates undergo a subcritical transition to turbulence. We carry out an extensive linear non-modal stability... -
Optimal perturbation (classic, Re=2000,A=1,Wo=15): Time series of the r-theta...
Laminar flows through pipes driven at steady, pulsatile or oscillatory rates undergo a subcritical transition to turbulence. We carry out an extensive linear non-modal stability... -
fac-tris[2-phenylpyridinato-C2,N]iridium(III)
fac-tris[2-phenylpyridinato-C2,N]iridium(III) (tris-(2-phenylpyridine) iridium, [Ir(ppy)3]), is a heavy metal complex that is the most frequently used precursor molecule for the... -
Investigating the structure of novel zinc and magnesium doped bioactive glasses
A range of novel bioactive glasses containing zinc and magnesium have recently been developed for dental and orthopaedic applications. At present little is known about the... -
Structure and Reaction Kinetics of Phenylacetylene Hydrogenation in a Porous ...
This project aims to study the confinement of phenyl acetylene in the pores of mesoporous titania catalysts for the conversion into styrene. Specifically, neutron scattering... -
Local structure study of Cr-Fe alloys with enhanced magnetovolume effect
Negative thermal expansion (NTE) materials, the volume of a material abnormally contract with the increase of temperature, is closed related to the magnetovolume effect in...
