A Principal Determinant in Cathodic Protection Design of Offshore Structures—The Mean Current Density

CORROSION ◽  
2000 ◽  
Vol 56 (10) ◽  
pp. 988-997 ◽  
Author(s):  
W. H. Hartt ◽  
E. Lemieux
CORROSION ◽  
10.5006/2492 ◽  
2017 ◽  
Vol 74 (1) ◽  
pp. 123-133 ◽  
Author(s):  
M.-S. Hong ◽  
J.-H. Hwang ◽  
J.H. Kim

The temperature effect on the current density which closely related to cathodic protection (CP) design was examined using electrochemical tests. A case study of an optimized CP design for the floating production storage and offloading using a computational analysis tool was also performed. The electrochemical test results showed that the current density and the surface resistance of the specimen (EH36) at 28°C are lower and higher, respectively, compared with the 5°C condition; this phenomenon is the result of a calcareous deposit that was verified by scanning electron microscopy and energy dispersive x-ray spectroscopy surface analyses. The polarization curves which contained the effect of calcareous deposits according to the temperature were used as the computational analysis input data. The simulation results showed that the structure under the 5°C condition did not satisfy the CP criteria (−800 mVSCE to −1,050 mVSCE) at the bottom shell and the mooring chain. It had higher potential than −800 mVSCE. Although the structure at 28°C satisfied the protective potential range, it was sufficiently unstable for the prediction of the corrosion damage. To optimize and resolve the identified problems, the CP design was changed by CP methods, anodes quantities, and anodes distribution. Consequently, the structure at 5°C is sufficient for the satisfaction of the protective-potential criteria (< −800 mVSCE) at the bottom shell and the mooring chain. In the case of the structure at 28°C, a more-even potential distribution was achieved.


2017 ◽  
Vol 8 (10) ◽  
pp. 6871-6880 ◽  
Author(s):  
Richard Stones ◽  
Hoda Hossein-Nejad ◽  
Rienk van Grondelle ◽  
Alexandra Olaya-Castro

We investigate the performance of a theoretical photosystem II reaction centre-inspired photocell device through the framework of electron counting statistics. In particular we look at the effect of a structured vibrational environment on the mean current and current noise.


CORROSION ◽  
1984 ◽  
Vol 40 (2) ◽  
pp. 88-92 ◽  
Author(s):  
J. D. Talati ◽  
G. A. Patel ◽  
D. K. Gandhi

2015 ◽  
Vol 45 (3) ◽  
pp. 613-629 ◽  
Author(s):  
M. Jeroen Molemaker ◽  
James C. McWilliams ◽  
William K. Dewar

AbstractThe California Undercurrent (CUC) flows poleward mostly along the continental slope. It develops a narrow strip of large negative vertical vorticity through the turbulent boundary layer and bottom stress. In several downstream locations, the current separates, aided by topographic curvature and flow inertia, in particular near Point Sur Ridge, south of Monterey Bay. When this happens the high-vorticity strip undergoes rapid instability that appears to be mesoscale in “eddy-resolving” simulations but is substantially submesoscale with a finer computational grid. The negative relative vorticity in the CUC is larger than the background rotation f, and Ertel potential vorticity is negative. This instigates ageostrophic centrifugal instability. The submesoscale turbulence is partly unbalanced, has elevated local dissipation and mixing, and leads to dilution of the extreme vorticity values. Farther downstream, the submesoscale activity abates, and the remaining eddy motions exhibit an upscale organization into the mesoscale, resulting in long-lived coherent anticyclones in the depth range of 100–500 m (previously called Cuddies) that move into the gyre interior in a generally southwestward direction. In addition to the energy and mixing effects of the postseparation instability, there is are significant local topographic form stress and bottom torque that retard the CUC and steer the mean current pathway.


2013 ◽  
Vol 66 (4) ◽  
pp. 507-512 ◽  
Author(s):  
Lorgio Gilberto Valdiviezo Gonzales ◽  
Gabriela Alejandra Huamán Pino ◽  
Maurício Leonardo Torem

In this work, the electroflotation of cassiterite fine ranges using Rhodococcus opacus (R. opacus) as bioreagent has been carried out. The interaction between R. opacus and mineral surface was valued through the zeta potential, contact angles measurements and adsorption studies. Furthermore, studies were attempted to check the effect of current density and microorganism concentration on mean bubble size (Sauter). After the interaction, the resulting particles exhibited hydrophobic characters, as verified by the increase of the contact angle. Also, the electrophoretic mobilities of cassiterite particles showed a mean value close to zero after interaction with R. opacus. The measurement of bubble size by laser diffraction showed a mean bubble size of 26µm. Current density and bacterial concentration seem to be the main parameters affecting the mean diameter of the bubbles. An electroflotation test reported recovery of around 64.5% at pH 5, concentration of 2.87x10¹² cells/ml (50 mg/L) and current density of 51.4 mA/cm².


2020 ◽  
Vol 19 ◽  

Cathodic protection is defined as a method for slowing down or complete elimination of corrosion processes on underground or underwater, insulated or uninsulated metal structures. Protection by cathodic protection system is achieved by polarizing protected object to more negative value, with respect to its equilibrium potential. Design of the cathodic protection system implies determination of the electric potential and current density on the electrode surfaces after installation of the cathodic protection system. Most efficient way for determination of the electric potential and current density in the cathodic protection system is by applying numerical techniques. When modeling cathodic protection systems by numerical techniques, electrochemical reactions that occur on electrode surfaces are taken into account by polarization characteristics. Because of nature of the electrochemical reactions, polarization characteristics are nonlinear and under certain conditions can be time – varying (dynamic nonlinear polarization characteristics). This paper deals with numerical modeling of the cathodic protection system with dynamic nonlinear polarization characteristics. Numerical model presented in this paper is divided in the two parts. First part, which is based on the direct boundary element method, is used for the calculation of the distribution of electric potential and current density on the electrode surfaces in the spatial domain. Second part of the model is based on the finite difference time domain method and is used for the calculation of the electric potential and current density change over time. The use of presented numerical model is demonstrated on two simple geometrically examples.


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