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Chilling Tendency and Chill of Cast Iron

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182<br />

The chilling tendency CT can be calculated from Eq.<br />

(7) as a function <strong>of</strong> the chemical composition <strong>of</strong> the<br />

cast iron, Ns <strong>and</strong> b, listed in Table 3, the mean temperature<br />

<strong>of</strong> the metal just after pouring, Ti≈1260℃, <strong>and</strong> any<br />

relevant thermophysical data (shown in Table 1).<br />

Table 4 shows results for plate-shape castings reported<br />

in the literature [4] with various chemical compositions<br />

<strong>and</strong> wall thicknesses, as well as the number <strong>of</strong><br />

nodules <strong>and</strong> the cementite fraction. In these cases, the<br />

nucleation coefficients b <strong>and</strong> Ns are not known, so CT<br />

is calulated using Eq. (8). The results in Table 4 show<br />

that in melts I <strong>and</strong> II, chill starts to occur in walls with<br />

thicknesses between 3 <strong>and</strong> 6 mm, while in melt III chill<br />

starts to occur for wall thicknesses between 1.5 <strong>and</strong> 2<br />

mm. scr must be calculated using Eq. (1) to compare<br />

these results with the theoretical predictions. These<br />

calculations assumed that a=0.11 J/(cm 2 ·s 1/2 · ℃ )<br />

<strong>and</strong> Ti=1250℃ with other information taken from Table<br />

1. The results in Table 4 show that in melt I the<br />

Tsinghua Science <strong>and</strong> Technology, April 2008, 13(2): 177-183<br />

change <strong>of</strong> the wall thickness, s, from 6 mm to 3 mm is<br />

closely linked to the change in the number <strong>of</strong> nodules<br />

from 588 to 1039 mm −2 . As a result, an average nodule<br />

count <strong>of</strong> NF,cr=813 mm −2 was used in this work. Similar<br />

determinations were made for melts II <strong>and</strong> III with NF,cr<br />

values <strong>of</strong> 945 <strong>and</strong> 1959 mm −2 , respectively. scr for<br />

melts I, II, <strong>and</strong> III were then 3.4 mm, 3.1 mm, <strong>and</strong><br />

1.8 mm as shown in Table 4. In addition, comparison<br />

<strong>of</strong> s <strong>and</strong> scr in Table 4 indicates that the predictions<br />

from the theoretical analysis are in good agreement<br />

with the experimental determinations <strong>of</strong> the wall thickness<br />

at which chill occurs. Table 4 shows the CT for<br />

the three melts calculated using Eq. (8) <strong>and</strong> data in Table<br />

1. The results in Table 4 show that as the chilling<br />

tendency increases from 0.34 to 0.68 s 1/2 ·℃ –1/3 , the<br />

critical wall thickness, scr, increases from 1.8 to<br />

3.4 mm.<br />

Table 4 Chemical composition, wall thicknesses, nodule count, cementite fraction, <strong>and</strong> chilling tendency for three<br />

ductile cast iron melts<br />

Melt<br />

No.<br />

C/% Si/% P/%<br />

I 3.40 2.70 0.046<br />

II 3.45 2.91 0.044<br />

III 3.31 4.42 0.051<br />

4 Conclusions<br />

Wall thickness (mm)<br />

Experimental s Calculated scr<br />

(1) A simple theoretical analysis is presented which<br />

predicts the chilling tendency <strong>and</strong> chill in flake graphite<br />

<strong>and</strong> ductile cast iron based on<br />

The chemical composition <strong>of</strong> the casting which<br />

for flake graphite cast iron is characterized by ∆Tsc,<br />

fγ, T, µ, Ncr or Ns, <strong>and</strong> b, <strong>and</strong> for ductile cast iron is<br />

characterized by ∆Tsc, D, Tl, Ncr or Ns <strong>and</strong> b;<br />

The inoculation <strong>and</strong> spheroidization method, the<br />

superheating temperature, <strong>and</strong> bath holding<br />

Nodule count<br />

(NF/mm −2 )<br />

Fraction <strong>of</strong><br />

cementite (%)<br />

CT/( s 1/2 ·℃ –1/3 )<br />

6.0 588 0.0 0.68<br />

3.4<br />

3.0<br />

1039 9.0 —<br />

2.0 1380 24.0 —<br />

1.5<br />

1311 34.0 —<br />

6.0 854 0.0 0.60<br />

3.1<br />

3.0<br />

1037 7.3 —<br />

2.0 1100 24.0 —<br />

6.0 1127 0.0 —<br />

3.0<br />

1726 0.0 —<br />

2.0 1890 0.0 0.34<br />

1.8<br />

1.5<br />

2027 9.3 —<br />

times as characterized by Ncr or Ns <strong>and</strong> b;<br />

Selected thermophysical data <strong>of</strong> the metal <strong>and</strong><br />

mold material as well as the metal temperature<br />

just after pouring into the mold.<br />

(2) Theoretical calculations <strong>of</strong> the width <strong>of</strong> the total<br />

chill in wedges for flake graphite <strong>and</strong> <strong>of</strong> the critical<br />

wall thickness for nodular cast iron compare well with<br />

experimental data.<br />

(3) The absolute values <strong>of</strong> the chilling tendency <strong>of</strong><br />

cast iron are calculated to range from 0.3 to<br />

1.1 s 1/2 ·℃ –1/3 .

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