<p>Zinc ferrite (ZnFe<sub>2</sub>O<sub>4</sub>) formation presents a challenge in Steelmaking Off-Gas Cleaning Systems hindering efficient Zn recovery. The kinetics of ZnFe<sub>2</sub>O<sub>4</sub> formation on iron oxide particles through gas–solid reactions were measured in a Drop-Tube Reactor under the industrial operating conditions of an electric arc furnace: temperature of 950&#xa0;°C to 1200&#xa0;°C, particle residence time of 4 to 7 seconds, Zn partial pressure of 5 × 10<sup>−4</sup> to 1 × 10<sup>−2</sup> atm, CO<sub>2</sub> partial pressure of 0.1 to 0.35 atm, and CO partial pressure of 2 × 10<sup>−4</sup> to 7 × 10<sup>−2</sup> atm. The nucleation and growth rate equation, with an Avrami parameter of 0.5, half-order dependence with respect to Zn, CO<sub>2</sub>, and CO partial pressures for Fe<sub>2</sub>O<sub>3</sub>, and 3/4, 1, and 1-order dependence with respect to Zn, CO<sub>2</sub>, and CO partial pressures for Fe<sub>3</sub>O<sub>4</sub>, respectively, well describes the ZnFe<sub>2</sub>O<sub>4</sub> formation kinetics on Fe<sub>2</sub>O<sub>3</sub> and Fe<sub>3</sub>O<sub>4</sub>. The following rate equations were developed, where the activation energy using Fe<sub>2</sub>O<sub>3</sub> and Fe<sub>3</sub>O<sub>4</sub> was 89 and 65 kJ mol<sup>−1</sup>, respectively:</p><p><InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\frac{\text{d}}{X}_{\rm H}{\text{d}}t=\left[939\times {e}^{\frac{-89000}{RT}}\times \left[{\left({p}_{\rm Zn}\times {p}_{{\rm CO}_{2}}\right)}^{0.5}-{\left(\frac{{p}_{\rm CO}}{{K}_{\rm H}}\right)}^{0.5}\right]\right]\times \left[0.5\left(1-{X}_{\rm H}\right)\left[-\text{Ln}{\left(1-{X}_{\rm H}\right)]}^{-1}\right]\right]\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mfrac> <mtext>d</mtext> <mi>X</mi> </mfrac> <mi mathvariant="normal">H</mi> </msub> <mtext>d</mtext> <mi>t</mi> <mo>=</mo> <mfenced close="]" open="["> <mn>939</mn> <mo>×</mo> <msup> <mrow> <mi>e</mi> </mrow> <mfrac> <mrow> <mo>-</mo> <mn>89000</mn> </mrow> <mrow> <mi mathvariant="italic">RT</mi> </mrow> </mfrac> </msup> <mo>×</mo> <mfenced close="]" open="["> <msup> <mrow> <mfenced close=")" open="("> <msub> <mi>p</mi> <mi mathvariant="normal">Zn</mi> </msub> <mo>×</mo> <msub> <mi>p</mi> <msub> <mi mathvariant="normal">CO</mi> <mn>2</mn> </msub> </msub> </mfenced> </mrow> <mrow> <mn>0.5</mn> </mrow> </msup> <mo>-</mo> <msup> <mrow> <mfenced close=")" open="("> <mfrac> <msub> <mi>p</mi> <mi mathvariant="normal">CO</mi> </msub> <msub> <mi>K</mi> <mi mathvariant="normal">H</mi> </msub> </mfrac> </mfenced> </mrow> <mrow> <mn>0.5</mn> </mrow> </msup> </mfenced> </mfenced> <mo>×</mo> <mfenced close="]" open="["> <mn>0.5</mn> <mfenced close=")" open="("> <mn>1</mn> <mo>-</mo> <msub> <mi>X</mi> <mi mathvariant="normal">H</mi> </msub> </mfenced> <mfenced close="]" open="["> <mo>-</mo> <mtext>Ln</mtext> <msup> <mrow> <mfenced close=")" open="("> <mn>1</mn> <mo>-</mo> <msub> <mi>X</mi> <mi mathvariant="normal">H</mi> </msub> </mfenced> <mrow> <mo stretchy="false">]</mo> </mrow> </mrow> <mrow> <mo>-</mo> <mn>1</mn> </mrow> </msup> </mfenced> </mfenced> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\frac{\text{d}}{X}_{\rm M}{\text{d}}t=\left[321\times {e}^{\frac{-65000}{RT}}\times \left[{\left({\left({p}_{\rm Zn}\right)}^{1.5}\times {\left({p}_{\text{CO}_{2}}\right)}^{2}\right)}^{0.5}-{\left(\frac{{\left({p}_{\rm CO}\right)}^{2}}{{K}_{\rm M}}\right)}^{0.5}\right]\right]\times \left[0.5\left(1-{X}_{\rm M}\right)\left[-\text{Ln}{\left(1-{X}_{\rm M}\right)]}^{-1}\right]\right]\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mfrac> <mtext>d</mtext> <mi>X</mi> </mfrac> <mi mathvariant="normal">M</mi> </msub> <mtext>d</mtext> <mi>t</mi> <mo>=</mo> <mfenced close="]" open="["> <mn>321</mn> <mo>×</mo> <msup> <mrow> <mi>e</mi> </mrow> <mfrac> <mrow> <mo>-</mo> <mn>65000</mn> </mrow> <mrow> <mi mathvariant="italic">RT</mi> </mrow> </mfrac> </msup> <mo>×</mo> <mfenced close="]" open="["> <msup> <mrow> <mfenced close=")" open="("> <msup> <mrow> <mfenced close=")" open="("> <msub> <mi>p</mi> <mi mathvariant="normal">Zn</mi> </msub> </mfenced> </mrow> <mrow> <mn>1.5</mn> </mrow> </msup> <mo>×</mo> <msup> <mrow> <mfenced close=")" open="("> <msub> <mi>p</mi> <msub> <mtext>CO</mtext> <mn>2</mn> </msub> </msub> </mfenced> </mrow> <mn>2</mn> </msup> </mfenced> </mrow> <mrow> <mn>0.5</mn> </mrow> </msup> <mo>-</mo> <msup> <mrow> <mfenced close=")" open="("> <mfrac> <msup> <mrow> <mfenced close=")" open="("> <msub> <mi>p</mi> <mi mathvariant="normal">CO</mi> </msub> </mfenced> </mrow> <mn>2</mn> </msup> <msub> <mi>K</mi> <mi mathvariant="normal">M</mi> </msub> </mfrac> </mfenced> </mrow> <mrow> <mn>0.5</mn> </mrow> </msup> </mfenced> </mfenced> <mo>×</mo> <mfenced close="]" open="["> <mn>0.5</mn> <mfenced close=")" open="("> <mn>1</mn> <mo>-</mo> <msub> <mi>X</mi> <mi mathvariant="normal">M</mi> </msub> </mfenced> <mfenced close="]" open="["> <mo>-</mo> <mtext>Ln</mtext> <msup> <mrow> <mfenced close=")" open="("> <mn>1</mn> <mo>-</mo> <msub> <mi>X</mi> <mi mathvariant="normal">M</mi> </msub> </mfenced> <mrow> <mo stretchy="false">]</mo> </mrow> </mrow> <mrow> <mo>-</mo> <mn>1</mn> </mrow> </msup> </mfenced> </mfenced> </mrow> </math></EquationSource> </InlineEquation>.</p><p>Under the studied conditions, Fe<sub>2</sub>O<sub>3</sub> conversion to ZnFe<sub>2</sub>O<sub>4</sub> is higher than that with Fe<sub>3</sub>O<sub>4</sub>. Maximizing Zn recovery while minimizing ZnFe<sub>2</sub>O<sub>4</sub> formation becomes possible through In-Process Separation by combining this rate equation with continuous <i>in situ</i> measurements.</p>

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Mechanism and Kinetics of Zinc Ferrite Formation in the EAF Off-Gas Cleaning System

  • John Frank Otero Olmos,
  • Hong Yong Sohn,
  • Naiyang Ma

摘要

Zinc ferrite (ZnFe2O4) formation presents a challenge in Steelmaking Off-Gas Cleaning Systems hindering efficient Zn recovery. The kinetics of ZnFe2O4 formation on iron oxide particles through gas–solid reactions were measured in a Drop-Tube Reactor under the industrial operating conditions of an electric arc furnace: temperature of 950 °C to 1200 °C, particle residence time of 4 to 7 seconds, Zn partial pressure of 5 × 10−4 to 1 × 10−2 atm, CO2 partial pressure of 0.1 to 0.35 atm, and CO partial pressure of 2 × 10−4 to 7 × 10−2 atm. The nucleation and growth rate equation, with an Avrami parameter of 0.5, half-order dependence with respect to Zn, CO2, and CO partial pressures for Fe2O3, and 3/4, 1, and 1-order dependence with respect to Zn, CO2, and CO partial pressures for Fe3O4, respectively, well describes the ZnFe2O4 formation kinetics on Fe2O3 and Fe3O4. The following rate equations were developed, where the activation energy using Fe2O3 and Fe3O4 was 89 and 65 kJ mol−1, respectively:

\(\frac{\text{d}}{X}_{\rm H}{\text{d}}t=\left[939\times {e}^{\frac{-89000}{RT}}\times \left[{\left({p}_{\rm Zn}\times {p}_{{\rm CO}_{2}}\right)}^{0.5}-{\left(\frac{{p}_{\rm CO}}{{K}_{\rm H}}\right)}^{0.5}\right]\right]\times \left[0.5\left(1-{X}_{\rm H}\right)\left[-\text{Ln}{\left(1-{X}_{\rm H}\right)]}^{-1}\right]\right]\) d X H d t = 939 × e - 89000 RT × p Zn × p CO 2 0.5 - p CO K H 0.5 × 0.5 1 - X H - Ln 1 - X H ] - 1 , \(\frac{\text{d}}{X}_{\rm M}{\text{d}}t=\left[321\times {e}^{\frac{-65000}{RT}}\times \left[{\left({\left({p}_{\rm Zn}\right)}^{1.5}\times {\left({p}_{\text{CO}_{2}}\right)}^{2}\right)}^{0.5}-{\left(\frac{{\left({p}_{\rm CO}\right)}^{2}}{{K}_{\rm M}}\right)}^{0.5}\right]\right]\times \left[0.5\left(1-{X}_{\rm M}\right)\left[-\text{Ln}{\left(1-{X}_{\rm M}\right)]}^{-1}\right]\right]\) d X M d t = 321 × e - 65000 RT × p Zn 1.5 × p CO 2 2 0.5 - p CO 2 K M 0.5 × 0.5 1 - X M - Ln 1 - X M ] - 1 .

Under the studied conditions, Fe2O3 conversion to ZnFe2O4 is higher than that with Fe3O4. Maximizing Zn recovery while minimizing ZnFe2O4 formation becomes possible through In-Process Separation by combining this rate equation with continuous in situ measurements.