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Acta Metall Sin  2019, Vol. 55 Issue (6): 801-810    DOI: 10.11900/0412.1961.2018.00562
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Reconstruction and Characterization of Galvanic Corrosion Behavior of X80 Pipeline Steel Welded Joints
Yadong LI1,Qiang LI2,Xiao TANG1,Yan LI1()
1. School of Materials Science and Engineering, China University of Petroleum (East China), Qingdao 266580, China
2. College of Pipeline and Civil Engineering, China University of Petroleum (East China), Qingdao 266580, China
Cite this article: 

Yadong LI,Qiang LI,Xiao TANG,Yan LI. Reconstruction and Characterization of Galvanic Corrosion Behavior of X80 Pipeline Steel Welded Joints. Acta Metall Sin, 2019, 55(6): 801-810.

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Abstract  

Welding is widely used for pipeline connection. Composition, microstructures and properties of the welded joints are highly heterogeneous and the resultant corrosion such as galvanic corrosion between different parts is widely present and influence the long-time service and safety. In this sense, the fundamental research in the electrochemical behavior of such joint parts is required. Electrochemical corrosion behavior of simulated X80 steel welded joint, accurately modeled by wire beam electrode (WBE) technique, was investigated by classical electrochemical techniques and microelectrode array (MEA) technique. A new index, namely the galvanic corrosion intensity factor, was proposed and verified to succeed in characterizing the degree of galvanic corrosion. Results showed that microstructure of granular bainite mixed with ferrite showed the highest positive open circuit potential and lowest polarization resistance. Furthermore, the corrosion tendency of the isolated electrodes that constituted the X80 steel welded joint was found to increase in the following order: fine grain heat affected zone (FGHAZ) < intercritical heat affected zone (ICHAZ) < base metal (BM) < coarse grain heat affected zone (CGHAZ) < weld metal (WM). Due to the difference in potential and the polarization characteristics, the WM displayed the highest polarization resistance but the most positive current density. The CGHAZ possessed a lower polarization resistance and a higher positive current density. In comparison, the FGHAZ and ICHAZ performed a lower polarization resistance but higher negative current densities. The WM and CGHAZ acted as the main anode, while the FGHAZ and ICHAZ acted as the main cathode and the galvanic current polarity of some BM electrodes changed with time during the immersion test. The intensity of galvanic corrosion of simulated X80 steel welded joint plateaued with immersion time. The results revealed that WM and CGHAZ were the weak links in the simulated X80 pipeline steel welded joints during its long-term service.

Key words:  pipeline steel      welded joint      galvanic corrosion      microelectrode array      reconstruction     
Received:  24 December 2018     
ZTFLH:  TG172  
Fund: National Natural Science Foundation of China(No.41676071);Fundamental Research Funds for the Central Universities(No.18CX05021A)

URL: 

https://www.ams.org.cn/EN/10.11900/0412.1961.2018.00562     OR     https://www.ams.org.cn/EN/Y2019/V55/I6/801

Fig.1  Schematics of accurate modeling of the welded joint (BM—base metal, HAZ—heat affected zone, WM—weld metal)
Fig.2  Microstructures of X80 steel (AF—acicular ferrite, MF—massive ferrite, QF—quasi-polygonal ferrite, M-A—
Fig.3  Open circuit potential (OCP) distribution of X80 steel welded joint
Fig.4  Nyquist diagram (a) and Bode plots (b) of X80 steel welded joint in NACE solution saturated with CO2 (NACE—national association of corrosion engineers)
Fig.5  Equivalent circuit for fitting EIS data (Rs—solution resistance, CPEf—capacitance of corrosion scale, Rpore—resistance of defects, Cdl—double layer capacitance, Rp—polarization resistance, RL—inductive resistance, L—inductance)

Region

Rs

Ω·cm2

Y0

S·sn·cm-2

n

Rpore

Ω·cm2

Rp

Ω·cm2

Cdl

μF·cm-2

L

H·cm-2

RL

Ω·cm2

BM4.11.5×10-30.67235319482110
ICHAZ0.72.3×10-30.6917283244970
FGHAZ1.01.7×10-30.6722382193473
CGHAZ1.01.4×10-30.68183521180280
WM2.78×10-40.73244720331267
Table 1  Fitting results of the EIS of X80 steel welded joint in NACE solution saturated with CO2
Fig.6  Polarization resistance of X80 steel welded joint at different immersion time
Fig.7  Potentiodynamic polarization curves of X80 steel welded joint
Fig.8  Potentiodynamic polarization curves of X80 steel (a), ICHAZ (b), FGHAZ (c), CGHAZ (d) and WM (e)

Time

h

Region

ba

mV·dec-1

bc

mV·dec-1

Ecorr

V

icorr

mA·cm-2

0.5BM72-181-0.6140.2345
ICHAZ77-188-0.6040.3421
FGHAZ86-183-0.6090.2921
CGHAZ66-177-0.6170.2913
WM64-174-0.6180.2195
2BM100-188-0.6380.1457
ICHAZ99-178-0.6260.2176
FGHAZ90-171-0.6210.2261
CGHAZ91-172-0.6230.2231
WM104-187-0.6470.1281
4BM106-189-0.6400.1423
ICHAZ108-190-0.6340.2107
FGHAZ101-187-0.6210.1954
CGHAZ109-189-0.6360.2403
WM114-181-0.6560.1269
6BM110-187-0.6430.1404
ICHAZ117-183-0.6380.2164
FGHAZ105-202-0.6360.2207
CGHAZ114-196-0.6420.2505
WM115-180-0.6550.1117
Table 2  Electrochemical parameters fitted from potentiodynamic polarization curves
  
Fig.10  Galvanic current density (ig) distribution of simulated welded joint
Fig.11  Galvanic effect (γ) of main anode and secondary anode in simulated welded joint at different immersion time
Fig.12  Values of galvanic corrosion intensity factor (g) and normalized maximum galvanic current density (ig,max) calculated from galvanic current as a function of time
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