Following Ramachandran 2: exit vector plot (EVP) analysis of disubstituted saturated rings

EVP analysis of common saturated rings revealed five regions (α–ε); only part of them corresponds to 3D molecular structures.

Abstract 17832: A New Rapid Vector Technique to Localize the PVC Origin From the 12-lead Ecg Compared to Cips

Introduction: Prior accurate PVC localization improves the time and outcome of ablative procedures. We developed a new manual Vector Technique (VcT) to localize the PVC origin to cardiac anatomy regions. In contrast, our Cardiac Isochrone Positioning System (CIPS) is a computer based system that localizes the PVC to patient specific cardiac anatomy from the MRI and electrode positions from the 3D Camera. Hypothesis: We hypothesize that this new VcT can rapidly quantitate the location of PVC to anatomical regions whereas CIPS localizes the PVCs to more specific cardiac anatomical segments. Method: The VcT assumes the frontal plane leads are formatted on the chest as an equilateral triangle and the horizontal leads as a partial sphere. Using the concept that a lead recording perpendicular to a dipole vector is zero, the QRS axis vectors of the PVC were calculated manually within 3.8 to 7.5 degrees in the frontal and horizontal planes. CIPS computed the electrode positions by registration of the MRI derived torso model with the 3D image of the patient. The ECG signals were used by both methods to localize the PVC origin to the cardiac anatomy. Result: In 12 patients (below), this manual VcT separated without overlap in the horizontal plane the PVC into Left Ventricle (LV 30-45°), Right Ventricular (RV 308-348°), and Papillary Muscle (PM 128-150°) regions, but not in the frontal plane. CIPS localized 10 PVCs to the same and 2 to adjacent anatomical segments while the vector technique cannot because of the need for a database to create a PVC anatomic segment model. Conclusion: This new VcT can be used by anyone to localize rapidly the PVC by a QRS vector plot to regions like the left & posterior for the RV, left & anterior for the LV, and right & anterior for the papillary muscles while CIPS can localize PVCs more specifically to anatomical segments. Using the 12 lead ECG, this VcT creates a quantitative cardiac anatomical segment model of PVC locations integrated into CIPS that can improve the accuracy of VcT.

Mixing Characteristics of Elliptical and Rectangular Subsonic Jets with Swirling Co-flow

This paper presents a computational analysis of effects of swirling co-flow and non-circular subsonic compressible inner jets on centerline velocity decay, mass entrainment and jet spreading rate. Three different exit shapes of elliptical, rectangular and circular inner jets were compared for three different co-flow conditions such as no co-flow, straight co-flow and swirling co-flow. Co-flow is issuing from a circular annular duct. Swirling co-flow is created in the co-flow duct by introducing a swirler with stationary angular vanes of 50° oblique to the jet axis. Reynolds number of inner jet is calculated based on its equivalent diameter as 200342. It is found that the swirling co-flow has strong influence on the boundary condition of inner jet and alters the major features of the jet such as jet potential core length, centerline velocity decay rate and jet spread rate. Streamwise corner vortices of different jet conditions have been captured using velocity vector plot to show the effect of swirling co-flow on the jet flow field. Swirling co-flow with elliptical inner jet exhibits higher velocity decay rate and jet spreading rate than the equivalent area circular and rectangular jet.

A Refined Estimate for the Damping Coefficient

In the “Peak Amplitude” method of resonance testing the total amplitude of vibration is plotted against frequency or (frequency). The method is unreliable for systems which are heavily damped and for systems with close natural frequencies (for both of which a vector plot such as that suggested by Kennedy and Pancu should be used) but for many systems it provides a rough guide to the resonance properties. One of the principal difficulties attending the analysis of the amplitude plots is to find which part of a given peak is due to the resonant mode and which to the off-resonant vibration. In the note a method is described for analysing a peak assuming that:— (i)only a single resonant mode is involved(ii)the contribution to the amplitude from the off-resonant vibration is constant in the neighbourhood of the peak.