Improving the Corrosion Behavior of Ductile Cast Iron in Sulphuric Acid by Heat Treatment


Figure 4  illustrates the linear relation between i p  and log acid concentration.  Figure 4



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improving-the-corrosion-behavior-of-ductile-cast-iron-in-sulphuric-acid-by-heat-treatment

Figure 4 
illustrates the linear relation between i

and log acid concentration. 
Figure 4:
Dependence of i
p
on logC
H2SO4
.
On the other hand, the effect of scan rate υ on the polarization curves of the specimen's Nos. 0-5 in 1.0 M H
2
SO
4
and at 30
º
C was evaluated as shown in 
Figure 5
. In all cases, it is observed that an increase in the scan rate enhances 
the anodic dissolution of the specimens and delays the attainment of passivity. Both, the peak potential, E
p
and peak 
current, i
p
increase with increasing the scan rate. The linear relationship between E
p
vs log υ is shown in 
Figure 6

These data could be explained on the basis that the time allowed to nucleate (or growth) of iron oxide crystals at its 
equilibrium potential is very short, and passivation is delayed until the nuclei have grown to the critical size required 
for passivation [25]. On the other hand, the relation between the peak current i
p
and the square root of scan rate is 
shown in 
Figure 7
. The linear relation between peak current i
p
vs υ
1/2 
indicates diffusion controlled process (limitation 
of the film formation).
Figure 5:
Potentiodynamic anodic polarization curves for specimen No. 0 in 2.0 M H
2
SO

at 30
º
C and at different scan rates.


Ibrahim MAM, et al.
Der Chemica Sinica, 2017, 8(6):513-523
Pelagia Research Library
518
Figure 6: 
Dependence of E
p
on log υ.
Figure 7:
The relationship between i
p
versus υ
1/2
.
The effect of so
lution temperature on the polarization profiles of the six specimens (0-5) in 1.0 M H
2
SO
4
has been 
studied over the temperature range from 30-70
º
C. The results are given in 
Figure 8 (a-c)
. An increase of solution 
temperature increases the active dissolution and delays the passivation. At temperature higher than 40
º
C, the anodic 
current density i
a
for the specimens except specimen No. 1 increases exponentially with the applied potential up to 
2000 mV without any sign for passivity. At 70
º
C, no passive region was observed for all the six specimens (

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