MOLTEN STEEL REFINING METHOD

Abstract

A molten steel refining method increases a circulating rate using an RH vacuum degassing apparatus. An immersion depth of an immersion tube into molten steel inside a vacuum tank or a circulating gas flow rate is determined such that a stirring power energy density ε for the molten steel meets the following formulae: ε = [371GT × ln{ 1 + (ρ.sub.LgH.sub.0/P)}]/W.sub.v, W.sub.v = (π.Math.D.sub.v.sup.2/4) × H.sub.0 × ρ.sub.L/1000, H.sub.0 = h.sub.v + L - h.sub.G, h.sub.v = (P.sub.0 - P)/(ρ.sub.Lg) + 1 -L, 1.35 × 10.sup.5 × D.sub.U/W.sub.V < ε < 2.1 × 10.sup.4.

Claims

1. A molten steel refining method using an RH vacuum degassing apparatus, wherein an immersion depth 1 of an immersion tube into molten steel inside a vacuum tank or a circulating gas flow rate G is determined such that a stirring power energy density ε for the molten steel expressed by the following Formulae (1) to (4) meets the following Formula (5): $\begin{array}{cc}\text{ε}=\left[371\text{GT}\times \text{ln}\left\{1+\left({\text{ρ}}_{\text{L}}{\text{gH}}_0/\text{P}\right)\right\}\right]/{\text{W}}_{\text{V}}& \text{­­­(1)}\end{array}$ $\begin{array}{cc}{\text{W}}_{\text{V}}=\left(\pi \cdot {\text{D}}_{\text{V}}{}^2/4\right)\times {\text{H}}_0\times {\text{ρ}}_{\text{L}}/1000.& \text{­­­(2)}\end{array}$ $\begin{array}{cc}{\text{H}}_0={\text{h}}_{\text{V}}+\text{L}-{\text{h}}_{\text{G}}& \text{­­­(3)}\end{array}$ $\begin{array}{cc}{\text{h}}_{\text{V}}=\left({\text{P}}_0-\text{P}\right)/\left({\text{ρ}}_{\text{L}}\text{g}\right)+1-\text{L}& \text{­­­(4)}\end{array}$ $\begin{array}{cc}1.35\times {10}^5\times {\text{D}}_{\text{U}}/{\text{W}}_{\text{V}}<\text{ε}<2.1\times {10}^4& \text{­­­(5)}\end{array}$ where the symbols represent the following: ε: the stirring power energy density (watt/ton) for the molten steel inside the vacuum tank, G: the circulating gas flow rate (Nm.sup.3/sec), T: a temperature (K) of the molten steel, ρ.sub.L: a density (kg/m.sup.3) of the molten steel, g: a gravitational acceleration (9.8 m/sec.sup.2), W.sub.v: a mass (ton) of the molten steel inside the vacuum tank, D.sub.v: an inside diameter (m) of the vacuum tank, H.sub.0: a height (m) from a position of a circulating gas blow-in nozzle to a bath surface of the molten steel inside the vacuum tank in a stationary state, P: a pressure (Pa) inside the vacuum tank, P.sub.0: an atmospheric pressure (101325 Pa), h.sub.v: a height (m) from the bath surface of the molten steel inside the vacuum tank in the stationary state to a bed, L: a height (m) from a lower end of the immersion tube to the bed, h.sub.G: a height (m) from the lower end of the immersion tube to the position of the circulating gas blow-in nozzle, 1: the immersion depth (m) of the immersion tube into the molten steel, and D.sub.u: an inside diameter (m) of a rising tube.

2. The molten steel refining method according to claim 1, wherein the immersion depth 1 of the immersion tube into the molten steel or the circulating gas flow rate G is determined such that the stirring power energy density ε meets the following Formula (6): $\begin{array}{cc}1.35\times {10}^5\times {\text{D}}_{\text{U}}/{\text{W}}_{\text{V}}<\text{ε}<1.0\times {10}^4& \text{­­­(6)}\end{array}$ .

Description

BRIEF DESCRIPTION OF DRAWINGS

[0028] FIG. 1 is a schematic vertical sectional view showing one example of an RH vacuum degassing apparatus.

[0029] FIG. 2 is an enlarged sectional view of the RH vacuum degassing apparatus showing a concept of the present invention.

[0030] FIG. 3 is a graph showing a relationship of a standardized circulating rate with a stirring power energy density ε for a fluid inside a vacuum tank in a water model experiment.

[0031] FIG. 4 is a graph showing a relationship between stirring power energy E and Q.sub.E/Q.sub.C that is a ratio of an actually measured molten steel circulating rate Q.sub.E to a calculated molten steel circulating rate Q.sub.C obtained using Formula (A) in RH vacuum degassing apparatuses varying in an immersion tube diameter and a vacuum tank inside diameter.

[0032] FIG. 5 is a graph showing a relationship between a rising tube diameter D.sub.U and minimum stirring power energy E.sub.min.

[0033] FIG. 6 is a graph showing a relationship of the ratio Q.sub.E/Q.sub.C between the calculated molten steel circulating rate Q.sub.C and the actually measured molten steel circulating rate Q.sub.E with the stirring power energy density ε for molten steel inside a vacuum tank in actual operation.

DESCRIPTION OF EMBODIMENT

[0034] Before the present invention is described below based on a preferred embodiment, first, a result of a study that led to the present invention will be described. FIG. 1 is a schematic vertical sectional view showing one example of an RH vacuum degassing apparatus used for a molten steel refining method as one embodiment of the present invention.

[0035] In FIG. 1, reference sign 1 is an RH vacuum degassing apparatus; 2 is a ladle; 3 is molten steel; 4 is slag; 5 is a vacuum tank; 6 is an upper tank; 7 is a lower tank; 8 is a rising-side immersion tube (rising tube); 9 is a descending-side immersion tube (descending tube); 10 is a circulating gas blow-in pipe; 11 is a duct; 12 is a raw material charging port; and 13 is a top-blowing lance. The vacuum tank 5 is composed of the upper tank 6 and the lower tank 7. The top-blowing lance 13 is a device through which an oxygen gas or a solvent is blown to be added to the molten steel inside the vacuum tank, and is installed at an upper part of the vacuum tank 5 while being able to move up and down inside the vacuum tank 5.

[0036] In the RH vacuum degassing apparatus 1, the ladle 2 containing the molten steel 3 is raised by a raising-lowering device (not shown), and the rising-side immersion tube 8 and the descending-side immersion tube 9 are immersed into the molten steel 3 inside the ladle. Then, air inside the vacuum tank 5 is discharged by an exhaust device (not shown) coupled to the duct 11 to depressurize the inside of the vacuum tank 5, and a circulating gas is blown into the rising-side immersion tube 8 through the circulating gas blow-in pipe 10. When the inside of the vacuum tank 5 is depressurized, the molten steel 3 inside the ladle rises in proportion to the difference between an atmospheric pressure and a pressure (a degree of vacuum) inside the vacuum tank and flows into the vacuum tank. At the same time, due to a gas lifting effect of the circulating gas blown in through the circulating gas blow-in pipe 10, the molten steel 3 rises through the rising-side immersion tube 8 along with the circulating gas and flows into the vacuum tank 5. Thereafter, the molten steel 3 forms a flow that returns to the ladle 2 via the descending-side immersion tube 9, or a so-called circulating flow, and thus undergoes refining by RH vacuum degassing. As the molten steel 3 is exposed to a depressurized atmosphere inside the vacuum tank, gas components in the molten steel move to the atmosphere inside the vacuum tank and a degassing reaction of the molten steel 3 progresses.

[0037] In a water model experiment simulating an RH vacuum degassing apparatus, we studied about increasing the circulating rate of molten steel by making various changes to operation conditions. Here, a water model was used for the following reason. Molten steel is heavy and highly viscous compared with water, while molten steel and water have almost the same kinetic viscosity. Therefore, when simulation is conducted on a full scale (scale ratio 1.0) using water, two dimensionless numbers, a Froude number and a Reynolds number, can be matched with those of molten steel. Thus, in a full-scale simulation method using water, a flow of molten steel can be reproduced in terms of the influence of the gravity, inertial force, and viscous force. As a result, we found that the circulating rate could be efficiently increased by controlling the energy density ε of power with which the circulating gas blown into the rising tube stirred the fluid inside the vacuum tank to be within an appropriate range.

[0038] The stirring power energy density ε for the molten steel inside the vacuum tank is represented by the following Formulae (1) to (4):

[00008]$\begin{array}{cc}\text{ε=}\left[371\text{GT}\times \text{1n}\left\{1+\left({\text{ρ}}_{\text{L}}{\text{gH}}_0/\text{P}\right)\right\}\right]/{\text{W}}_{\text{V}}& \text{­­­(1)}\end{array}$

[00009]$\begin{array}{cc}{\text{W}}_{\text{V}}=\left(\text{π}\cdot {\text{D}}_{\text{V}}{}^2/4\right)\times {\text{H}}_0\times {\text{ρ}}_{\text{L}}/1000& \text{­­­(2)}\end{array}$

[00010]$\begin{array}{cc}{\text{H}}_0={\text{h}}_{\text{V}}+\text{L}\text{−}{\text{h}}_{\text{G}}& \text{­­­(3)}\end{array}$

[00011]$\begin{array}{cc}{\text{h}}_{\text{V}}=\left({\text{P}}_0-\text{P}\right)/\left({\text{ρ}}_{\text{L}}\text{g}\right)+1-\text{L}& \text{­­­(4)}\end{array}$

where the symbols represent the following: [0039] ε: the stirring power energy density (watt/ton) for the molten steel inside the vacuum tank, [0040] G: the circulating gas flow rate (Nm.sup.3/sec), [0041] T: the temperature (K) of the molten steel, [0042] ρ.sub.L: the density (kg/m.sup.3) of the molten steel, [0043] g: the gravitational acceleration (9.8 m/sec.sup.2), [0044] W.sub.v: the mass (ton) of the molten steel inside the vacuum tank, [0045] D.sub.v: the inside diameter (m) of the vacuum tank, [0046] H.sub.0: the height (m) from the position of a circulating gas blow-in nozzle to the bath surface of the molten steel inside the vacuum tank in the stationary state, [0047] P: the pressure (Pa) inside the vacuum tank, [0048] P.sub.0: the atmospheric pressure (101325 Pa), [0049] h.sub.v: the height (m) from the bath surface of the molten steel inside the vacuum tank in the stationary state to a bed, [0050] L: the height (m) from the lower end of the immersion tube to the bed, [0051] h.sub.G: the height (m) from the lower end of the immersion tube to the position of the circulating gas blow-in nozzle, and [0052] 1: the immersion depth (m) of the immersion tube into the molten steel.

[0053] FIG. 2 is an enlarged sectional view of the RH vacuum degassing apparatus representing the concept of the present invention. In FIG. 2, the symbols relating to the dimensions of the RH vacuum degassing apparatus used in the above Formulae (1) to (4) are indicated.

[0054] In Formula (4), the immersion depth 1 of the immersion tube into the molten steel is defined by the following Formula (B):

[00012]$\begin{array}{cc}1=1_{\text{L}}-1_{\text{FB}}-1_{\text{LV}}& \text{­­­(B)}\end{array}$

where, 1.sub.L: the distance (m) from the upper end of the ladle to the bottom of the ladle, [0055] 1.sub.FB: the distance (m) from the upper end of the ladle to the surface of the molten steel inside the ladle, and [0056] 1.sub.LV: the distance (m) from the lower end of the immersion tube to the bottom of the ladle. [0057] 1.sub.FB is obtained, for example, by measuring the surface level of the molten steel using a molten steel level meter, or by immersing a metal rod into the molten steel inside the ladle and measuring the length of a melted portion. 1.sub.LV is obtained from the relative distance between the ladle and the vacuum tank that is acquired from a control system.

[0058] In the water model experiment, the depth of water bath inside the vacuum tank was changed to various depths and the circulating rates at the respective water levels were obtained by measuring the flow velocity in the descending tube. FIG. 3 shows a relationship of a standardized circulating rate with the stirring power energy density ε for the fluid inside the vacuum tank in the water model experiment. The standardized circulating rate is a ratio relative to a value at which the circulating rate is lowest. As a result of the experiment, we found that when the circulating gas flow rate was constant, the circulating rate increased as the stirring power energy density ε for the fluid inside the vacuum tank decreased.

[0059] The reason why the circulating rate varies as described above is as follows: when the stirring power energy density ε for the molten steel inside the vacuum tank is lower, there is less stirring of the bath surface and the ratio of energy consumed as energy that fluctuates the boundary of the molten steel becomes lower, so that the ratio of a part of the energy of the circulating gas that contributes to circulation increases proportionally and thus the circulating rate increases.

[0060] Even when the stirring power energy density ε for the molten steel inside the vacuum tank is sufficiently low, if stirring power energy E (watt) expressed by the following Formula (C) is low relative to the inside diameter D.sub.U [0061] (m) of the rising tube, a lifting and pumping effect is not sufficiently exhibited and the circulating rate decreases.

[00013]$\begin{array}{cc}\text{E}\text{=}\left[371\text{GT}\times \text{1n}\left\{1+\left({\text{ρ}}_{\text{L}}{\text{gH}}_0/\text{P}\right)\right\}\right]\left(=\text{ε}\cdot {\text{W}}_{\text{V}}\right)& \text{­­­(C)}\end{array}$

[0062] FIG. 4 shows a relationship between the stirring power energy E and Q.sub.E/Q.sub.C that is a ratio of the actually measured molten steel circulating rate Q.sub.E (molten steel m.sup.3/min) to the calculated molten steel circulating rate Q.sub.C obtained using Formula (A) in RH vacuum degassing apparatuses varying in an immersion tube diameter and a vacuum tank inside diameter. For the actually measured molten steel circulating rate Q.sub.E, copper was added as a tracer from the vacuum tank during treatment and a homogeneous mixing time τ (sec) was measured, and the rate Q.sub.E was calculated from the obtained homogeneous mixing time τ using a relational expression to be described later. Formula (A) was calculated with the constant K set to 446.3. When the stirring power energy E is within a range equal to or higher than a certain value, as the stirring power energy E decreases, the stirring power energy density ε for the molten steel inside the vacuum tank also decreases, so that the energy efficiency increases and the circulating rate increases. On the other hand, when the stirring power energy E is equal to or lower than a certain value E.sub.min, the lifting and pumping effect of the gas falls short relative to the rising tube diameter D.sub.U, which leads to poor circulation and a decrease in Q.sub.E/Q.sub.C. Here, FIG. 5 shows a relationship between the rising tube diameter D.sub.U and E.sub.min, with E.sub.min defined as the minimum stirring power energy. From a proportional constant in proportional approximation of the relationship between the rising tube diameter D.sub.U and E.sub.min obtained from the relationship of FIG. 5, a condition for the stirring power energy E required for normal circulation in the RH vacuum degassing apparatus was defined as expressed by the following Formula (7):

[00014]$\begin{array}{cc}1.35\times {10}^5\times {\text{D}}_{\text{U}}\le \text{E}& \text{­­­(7)}\end{array}$

[0063] Using the relationship ε = E/W.sub.v, Formula (7) is transformed into the following Formula (8):

[00015]$\begin{array}{cc}1.35\times {10}^5\times {\text{D}}_{\text{U}}/{\text{W}}_{\text{V}}<\text{ε}& \text{­­­(8)}\end{array}$

[0064] Further, as a result of measuring the circulating rates under various conditions and evaluating Q.sub.E/Q.sub.C for the same RH vacuum degassing apparatus, we found that when the stirring power energy density ε for the molten steel inside the vacuum tank was lower than 2.1 × 10.sup.4, Q.sub.E/Q.sub.C increased greatly and exceeded 1.1. FIG. 6 shows the relationship between the stirring power energy density ε for the molten steel inside the vacuum tank and Q.sub.E/Q.sub.C. In FIG. 6, those conditions that do not meet Formula (8) are omitted.

[0065] From this result, Formula (9) is obtained as a condition for ε that increases the circulating rate:

[00016]$\begin{array}{cc}\text{ε<2}\text{.1}\times \text{1}{\text{0}}^4& \text{­­­(9)}\end{array}$

[0066] From Formula (8) and Formula (9), Formula (5) is obtained as a condition for the stirring power energy density ε required to increase the energy efficiency of the circulating gas and increase the circulating rate:

[00017]$\begin{array}{cc}1.35\times {10}^5\times {\text{D}}_{\text{U}}/{\text{W}}_{\text{V}}<\text{ε<2}\text{.1}\times \text{1}{\text{0}}^4& \text{­­­(5)}\end{array}$

[0067] When the stirring power energy density ε for the molten steel inside the vacuum tank is further decreased within a range that meets Formula (7), Q.sub.E/Q.sub.C increases further, and when ε is in a range lower than 1.0 × 10.sup.4, this ratio exceeds 1.2. Therefore, setting the value of ε to be lower than 1.0 × 10.sup.4 is more desirable. These conditions are expressed by a formula as by Formula (6):

[00018]$\begin{array}{cc}1.35\times {10}^5\times {\text{D}}_{\text{U}}/{\text{W}}_{\text{V}}<\text{ε<1}\text{.0}\times \text{1}{\text{0}}^4& \text{­­­(6)}\end{array}$

[0068] Parameters for controlling the stirring power energy density ε inside the vacuum tank to be within the range of Formula (5) or Formula (6) are the circulating gas flow rate G, the degree of vacuum P, and the immersion depth 1 of the immersion tube into the molten steel, other than the dimensions of the apparatus. When the degree of vacuum is degraded, the reaction speed of degassing that is the original purpose decreases or becomes zero. Therefore, it is desirable to perform control by changing the circulating gas flow rate G or the immersion depth 1 of the immersion tube into the molten steel.

[0069] As has been described above, the present invention can increase the circulating rate of molten steel without requiring new equipment investment or causing an increase in the treatment cost.

Examples

[0070] Vacuum refining of 300 tons of molten steel that had been blown by a converter was performed using an RH vacuum degassing apparatus. In this case, ε was calculated by Formulae (1) to (4) from the dimensions of the apparatus and operation conditions, and the immersion depth 1 of the immersion tube into the molten steel was adjusted within a range of 0.3 m to 0.9 m so as to meet Formula (5) or Formula (6). As the degassing tank, a degassing tank (tank A) having the vacuum tank cross-sectional area S.sub.A of 3.14 m.sup.2 and the rising tube inside diameter D.sub.U of 0.6 m, or the degassing tank (tank B) having a vacuum tank cross-sectional area S.sub.A of 3.8 m.sup.2 and the rising tube inside diameter D.sub.U of 0.8 m was used. As for the operation conditions, the degree of vacuum P was 133 Pa, and the circulating gas flow rate G was held constant at the flow rate of one of 0.020 Nm.sup.3/sec, 0.027 Nm.sup.3/sec, 0.037 Nm.sup.3/sec, and 0.050 Nm.sup.3/sec during treatment. Copper was added as a tracer from the vacuum tank into a circulating flow, and a homogeneous mixing time τ (sec) was measured and the actually measured molten steel circulating rate Q.sub.E was calculated from the obtained homogeneous mixing time τ. The relationship between the homogeneous mixing time τ and the actually measured molten steel circulating rate Q.sub.E is expressed by the following Formulae (D), (E), and (F):

[00019]$\begin{array}{cc}\text{τ=800}\times {\text{ε}}^{-0.45}& \text{­­­(D)}\end{array}$

[00020]$\begin{array}{cc}{\text{ε}}_{\text{L}}=8.33\times {10}^{-3}\times \text{ρ}{\text{Q}}_{\text{E}}{\text{v}}^2/{\text{W}}_{\text{L}}& \text{­­­(E)}\end{array}$

[00021]$\begin{array}{cc}\text{v}\text{=}{\text{Q}}_{\text{E}}/\left(15\text{π}{\text{D}}^2\right)& \text{­­­(F)}\end{array}$

where, ε.sub.L is the stirring power density (watt/ton) for the molten steel in the ladle, v is the flow velocity (m/sec) of the molten steel in the descending tube, and W.sub.L is the amount (ton) of the molten steel in the ladle.

[0071] Further, the calculated molten steel circulating rate Q.sub.C was obtained using Formula (A), and Q.sub.E/Q.sub.C was calculated for each charge. The constant K in Formula (A) was set to 446.3. The molten steel used had an element composition with C: 0.04 to 0.06 mass%, Si: 0.05 mass% or less, Mn: 0.3 mass% or less, P: 0.02 mass% or less, and S: 0.003 mass% or less, and the temperature of the molten steel before treatment was 1640 to 1670° C.

[0072] The result of the experiment is shown in Table 1. Within a range that meets Formula (5), the ratio of the actually measured molten steel circulating rate Q.sub.E to the calculated molten steel circulating rate Q.sub.C is equal to or higher than 1.1, regardless of differences in various operation conditions and the dimensions of the apparatus, which is a good result. Moreover, within a range that meets Formula (6), compared with when only Formula (5) is met, the circulating rate is further increased and Q.sub.E/Q.sub.C is stably equal to or higher than 1.2, which is an even better result.

TABLE-US-00001 No. G S.sub.A L h.sub.G l H.sub.0 h.sub.v D.sub.U V E ε Q.sub.E/Q.sub.C Remarks Nm.sup.3/sec m.sup.2 m m m m m m m.sup.3 watt watt/ton - 1 0.027 3.14 1.60 0.30 0.40 1.57 0.27 0.60 0.86 124728 20548 1.12 Inventive Example 2 0.027 3.14 1.60 0.30 0.45 1.62 0.32 0.60 1.02 126364 17466 1.14 Inventive Example 3 0.027 3.14 1.60 0.30 0.60 1.77 0.47 0.60 1.49 127380 12104 1.16 Inventive Example 4 0.027 3.14 1.60 0.30 0.70 1.87 0.57 0.60 1.81 128343 10078 1.19 Inventive Example 5 0.027 3.14 1.60 0.30 0.80 1.97 0.67 0.60 2.12 128806 8649 1.22 Inventive Example 6 0.027 3.14 1.60 0.30 0.85 2.02 0.72 0.60 2.28 129258 8082 1.21 Inventive Example 7 0.027 3.14 1.60 0.30 0.90 2.07 0.77 0.60 2.43 171501 7587 1.24 Inventive Example 8 0.037 3.80 1.60 0.30 0.45 1.62 0.32 0.80 1.23 173023 19847 1.15 Inventive Example 9 0.037 3.80 1.60 0.30 0.55 1.72 0.42 0.80 1.61 173751 15309 1.17 Inventive Example 10 0.037 3.80 1.60 0.30 0.60 1.77 0.47 0.80 1.80 175147 13754 1.18 Inventive Example 11 0.037 3.80 1.60 0.30 0.70 1.87 0.57 0.80 2.18 176471 11453 1.18 Inventive Example 12 0.037 3.80 1.60 0.30 0.80 1.97 0.67 0.80 2.56 177109 9829 1.20 Inventive Example 13 0.037 3.80 1.60 0.30 0.85 2.02 0.72 0.80 2.75 177730 9184 1.22 Inventive Example 14 0.037 3.80 1.60 0.30 0.90 2.07 0.77 0.80 2.95 235940 8621 1.23 Inventive Example 15 0.050 3.80 1.60 0.30 0.55 1.72 0.42 0.80 1.61 236933 20876 1.12 Inventive Example 16 0.050 3.80 1.60 0.30 0.60 1.77 0.47 0.80 1.80 237898 18756 1.15 Inventive Example 17 0.050 3.80 1.60 0.30 0.65 1.82 0.52 0.80 1.99 238837 17038 1.15 Inventive Example 18 0.050 3.80 1.60 0.30 0.70 1.87 0.57 0.80 2.18 239752 15617 1.14 Inventive Example 19 0.050 3.80 1.60 0.30 0.75 1.92 0.62 0.80 2.37 240643 14422 1.15 Inventive Example 20 0.050 3.80 1.60 0.30 0.80 1.97 0.67 0.80 2.56 241512 13403 1.17 Inventive Example 21 0.050 3.80 1.60 0.30 0.85 2.02 0.72 0.80 2.75 93111 12523 1.16 Inventive Example 22 0.020 3.14 1.60 0.30 0.40 1.57 0.27 0.60 0.86 94773 15411 1.17 Inventive Example 23 0.020 3.14 1.60 0.30 0.60 1.77 0.47 0.60 1.49 95535 9078 1.21 Inventive Example 24 0.020 3.14 1.60 0.30 0.70 1.87 0.57 0.60 1.81 96257 7559 1.22 Inventive Example 25 0.020 3.14 1.60 0.30 0.80 1.97 0.67 0.60 2.12 123551 6487 1.23 Inventive Example 26 0.027 3.14 1.60 0.30 0.35 1.52 0.22 0.60 0.71 123551 24999 1.01 Comparative Example 27 0.027 3.14 1.60 0.30 0.38 1.55 0.25 0.60 0.80 123912 22119 1.03 Comparative Example 28 0.037 3.80 1.60 0.30 0.35 1.52 0.22 0.80 0.85 169882 28408 0.99 Comparative Example 29 0.037 3.80 1.60 0.30 0.40 1.57 0.27 0.80 1.04 170704 23350 1.01 Comparative Example 30 0.050 3.80 1.60 0.30 0.40 1.57 0.27 0.80 1.04 232779 31841 0.97 Comparative Example 31 0.050 3.80 1.60 0.30 0.50 1.67 0.37 0.80 1.42 234918 23559 0.99 Comparative Example 32 0.020 3.14 1.60 0.30 0.70 1.87 0.57 0.80 1.81 95535 7559 0.82 Comparative Example

INDUSTRIAL APPLICABILITY

[0073] The molten steel refining method of the present invention can optimize the circulating rate in an RH vacuum degassing apparatus and thereby efficiently perform vacuum decarburization or vacuum degassing, which makes it useful for industrial purposes.

TABLE-US-00002 Reference Signs List 1 RH vacuum degassing apparatus 2 Ladle 3 Molten steel 4 Slag 5 Vacuum tank 6 Upper tank 7 Lower tank 8 Rising-side immersion tube (rising tube) 9 Descending-side immersion tube (descending tube) 10 Circulating gas blow-in pipe 11 Duct 12 Raw material charging port 13 Top-blowing lance