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Patent · US11331718B2 · B2 · US

Method for conveying container, device for conveying container, and method for conveying ladle

(11) Publication number
US11331718B2
(21) Application number
16/488,412
(22) Filing date
2017-12-11
(30) Priority date
2017-02-27
(43) Publication date
2022-05-17
(45) Date of grant
2022-05-17
(51) IPC
B22D 41/06; B22D 41/12; B65G 35/06; B65G 43/00
(52) CPC
  • B22D Casting of metals; casting of other substances by the same processes or devices: 41/12, 41/06
  • B65B Machines, apparatus or devices for, or methods of, packaging articles or materials; unpacking: 57/00
  • B65G Transport or storage devices, e.g. conveyors for loading or tipping, shop conveyor systems or pneumatic tube conveyors: 2813/023, 35/06, 43/00
(73) Assignee
Hitachi Metals Ltd
(72) Inventors
Takuya Harada
(54) Title
Method for conveying container, device for conveying container, and method for conveying ladle
(57) Abstract

A method for calculating a conveyance velocity at which oscillation of a liquid surface is suppressed in conveying a container in which a liquid is accommodated, e.g., a ladle in which molten metal is accommodated. In a graph of conveyance velocity versus conveyance time, an upwardly convex parabola and a downwardly convex parabola having vertical symmetry are prepared in advance, the downwardly convex parabola and the upwardly convex parabola are smoothly connected to form an acceleration curve, the upwardly convex parabola and the downwardly convex parabola are smoothly connected to form a deceleration curve, and the conveyance velocity is obtained from the acceleration curve and the deceleration curve smoothly connected where the slope thereof is zero.

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Claims (8)

  1. A method for conveying a container, comprising: starting a conveyance by accelerating the container containing a liquid in a horizontal direction; and decelerating the container to complete the conveyance, wherein a conveyance velocity v(t) of the container, which is a function of time t, is represented by: Formula 1 when 0≤t≤(t 0 /4) v (t)= a·t 2 [Formula 1] Formula 2 when (t 0 /4)≤t≤(3t 0 /4) v ⁡ (t) = - a · [(t - t 0 2) 2 - t 0 2 8] [Formula ⁢ ⁢ 2] Formula 3 when (3t 0 /4)≤t≤(t 0) v (t)= a ·(t−t 0) 2 [Formula 3] wherein ‘t 0 ’ represents a time for conveying the container and ‘a’ represents a constant, and the method further comprises determining the conveyance velocity v(t) of the container by using Formulae 1 to 3, and driving a motor that rotates a plurality of wheels of a trolley on which the container is placed and conveying the container in accordance with the determined conveyance velocity v(t) such that liquid surface oscillations after conveying the container are within a tolerable range.
  2. The method for conveying a container according to claim 1, wherein: the conveyance velocity v(t) of the container, which is a function of time t, is also represented by: Formula 4 when 0≤t≤(t 1 /4) v (t)= b·t 2 [Formula 4] Formula 5 when (t 1 /4)≤t≤(t 1 /2) v ⁡ (t) = - b · [(t - t 1 2) 2 - t 1 2 8] [Formula ⁢ ⁢ 5] Formula 6 when (t 1 /2)≤t≤(t 1 /2)+t 2 v ⁡ (t) = 1 8 ⁢ b · t 1 2 [Formula ⁢ ⁢ 6] Formula 7 when (t 1 /2)+t 2 ≤t≤(3t 1 /4)+t 2 v ⁡ (t) = - b · [(t - t 1 2 - t 2) 2 - t 1 2 8] [Formula ⁢ ⁢ 7] Formula 8 when (3t 1 /4)+t 2 ≤t≤t 1 +t 2 v (t)= b ·(t−t 1 −t 2) 2 [Formula 8] wherein ‘t 1 ’ represents a total time for conveying the container in acceleration and in deceleration, ‘t 2 ’ represents a time for conveying the container at a constant speed, and ‘b’ represents a constant, and the method further comprises: setting the conveyance time v(t) of the container by using Formulae 1 to 3 when a maximum value of the conveyance velocity v(t) among Formulae 1 to 3 is equal to or less than a velocity limit V max for the container, which is tolerable in conveying the container; and setting the conveyance time v(t) of the container by using Formulae 4 to 8 and calculating the conveyance time t 1 and the conveyance time t 2 from the constant a, the velocity limit V max, and a conveyance distance L of the container where the constant b is equal to the constant a and the constant speed of Formula 6 is the velocity limit V max when the maximum value of the conveyance velocity v(t) among Formulae 1 to 3 is more than the velocity limit V max.
  3. The method for conveying a container according to claim 2, wherein the liquid is a molten metal and the container is a tilting ladle.
  4. The method for conveying a container according to claim 1, wherein the constant a is determined α max /2 wherein α max represents a maximum value of a rate of change of acceleration of the container at which liquid surface oscillations after conveying the container is suppressed within a tolerable range.
  5. The method for conveying a container according to claim 4, wherein a conveyance distance of the container is L and a velocity limit of the container that is tolerable in conveying the container is V max; the conveyance velocity v(t) of the container is set by Formulae 1 to 3 when a maximum value of the conveyance velocity v(t) among Formula 1 to 3 is equal to or less than the velocity limit V max; and when the maximum value of the conveyance velocity v(t) among Formulae 1 to 3 is more than the velocity limit V max, a total time for conveying the container in acceleration and in deceleration is t 1, a time for conveying the container at a constant speed is t 2, and the constant is b, and, in addition, the conveyance velocity v (t) of the container, which is a function of time t, is represented by: Formula 4 when 0≤t≤(t 1 /4) v (t)= b·t 2 [Formula 4] Formula 5 when (t 1 /4)≤t≤(t 1 /2) v ⁡ (t) = - b · [(t - t 1 2) 2 - t 1 2 8] [Formula ⁢ ⁢ 5] Formula 6 when (t 1 /2)≤t≤(t 1 /2)+t 2 v ⁡ (t) = 1 8 ⁢ b · t 1 2 [Formula ⁢ ⁢ 6] Formula 7 when (t 1 /2)+t 2 ≤t≤(3t 1 /4)+t 2 v ⁡ (t) = - b · [(t - t 1 2 - t 2) 2 - t 1 2 8] [Formula ⁢ ⁢ 7] Formula 8 when (3t 1 /4)+t 2 ≤t≤t 1 +t 2 v (t)= b ·(t−t 1 −t 2) 2 [Formula 8] wherein the conveyance velocity v(t) is set from the conveyance time t 1 and the conveyance time t 2 that are calculated from the constant a, the velocity limit V max, and the conveyance distance L where the constant b is the constant a and the constant speed of Formula 6 is the velocity limit V max.
  6. The method for conveying a container according to claim 1, wherein the liquid is a molten metal and the container is a tilting ladle.
  7. A conveyor control device for conveying a container, which starts conveying by accelerating the container containing a liquid in a horizontal direction and completes the conveyance after deceleration, the conveyor control device comprising: a computer, wherein the computer stores a conveyance time t 0 of the container, a constant a, a maximum value of a rate of change of acceleration of the container α max at which liquid surface oscillations after conveying the container are suppressed within a tolerable range; the computer also stores a conveyance velocity of the container v(t), which is a function of time t as: Formula 1 when 0≤t≤(t 0 /4) v (t)= a·t 2 [Formula 1] Formula 2 when (t 0 /4)≤t≤(3t 0 /4) v ⁡ (t) = - a · [(t - t 0 2) 2 - t 0 2 8] [Formula ⁢ ⁢ 2] Formula 3 when (3t 0 /4)≤t≤(t 0) v (t)= a ·(t−t 0) 2 [Formula 3] the computer is programmed to calculate the constant a from the stored rate of change of acceleration α max and determine the conveyance velocity v(t) of the container by using Formulae 1 to 3; and the computer is programmed to drive a motor that rotates a plurality of wheels of a trolley on which the container is placed and convey the container in accordance with the determined conveyance velocity v(t) such that the liquid surface oscillations after conveying the container are within the tolerable range.
  8. The conveyor control device unit for conveying a container according to claim 7, wherein the computer stores a conveyance distance L, a velocity limit V max for the container, which is tolerable in conveying the container, a total time t 1 for the container to be conveyed in acceleration and deceleration, a constant speed time t 2, and a constant b; the computer also stores the conveyance velocity of the container v(t), which is a function of time t as: Formula 4 when 0≤t≤(t 1 /4) v (t)= b·t 2 [Formula 4] Formula 5 when (t 1 /4)≤t≤(t 1 /2) v ⁡ (t) = - b · [(t - t 1 2) 2 - t 1 2 8] [Formula ⁢ ⁢ 5] Formula 6 when (t 1 /2)≤t≤(t 1 /2)+t 2 v ⁡ (t) = 1 8 ⁢ b · t 1 2 [Formula ⁢ ⁢ 6] Formula 7 when (t 1 /2)+t 2 ≤t≤(3t 1 /4)+t 2 v ⁡ (t) = - b · [(t - t 1 2 - t 2) 2 - t 1 2 8] [Formula ⁢ ⁢ 7] Formula 8 when (3t 1 /4)+t 2 ≤t≤t 1 +t 2 v (t)= b ·(t−t 1 −t 2) 2 [Formula 8] and when a maximum value of the conveyance velocity v(t) among Formulae 1 to 3 is equal to or less than the velocity limit V max, the computer is programmed to set the conveyance time v(t) of the container by using Formulae 1 to 3; and when the maximum value of the conveyance velocity v(t) among Formulae 1 to 3 is more than the velocity limit V max, the computer is programmed to set the conveyance time v(t) of the container by using Formulae 4 to 8, and, in addition, the computer is programmed to calculate the conveyance time t 1 and the conveyance time t 2 from the constant a, the velocity limit V max, and the conveyance distance L where the constant b is equal to the constant a and the constant speed of Formula 6 is the velocity limit V max.

Description

The present invention relates to a method for conveying a container containing a liquid, and more particularly to a method for conveying a ladle containing molten metal.

An example of conveyance of a container containing a liquid is a conveyance of a ladle in a casting line. During this conveyance, after the ladle is conveyed to a pouring position, oscillations may be generated on a surface of molten metal in the ladle. If such oscillations continue for a long time, measurement of the ladle weight becomes unstable, which may affect feeding accuracy of the molten metal.

It has been known that such oscillations of a liquid surface can be suppressed by making a curve of acceleration and deceleration in a graph of velocity versus time of ladle conveyance an S shape. It has been also known that such an S-shaped curve can be calculated from a liquid simulation (Patent Document 1 for example).

As described in Patent Document 1, the calculation of the curve from a liquid simulation requires complex calculations using a plurality of parameters, such as conditions of the ladle and the molten metal, conveyance distance, conveyance time, and so on. However, it is often required in a casting line to change a ladle for another or to change the conveyance distance according to positions of molds. In such cases, it is required to change the above parameters according to the conditions and to do the complex calculations over again. That is, applying a liquid simulation to a conveyance of a ladle in a casting line may complicate setting of the conveyance velocity.

Citations (8)

  • JPS51105017U
  • US4491074A
  • JPH0910924A
  • JPH09277025A
  • JP2006283786A
  • US8062578B2
  • WO2014174977A1
  • US20170217695A1
Record as JSON
{
  "publication_number": "US11331718B2",
  "country": "US",
  "kind": "B2",
  "title": "Method for conveying container, device for conveying container, and method for conveying ladle",
  "abstract": "A method for calculating a conveyance velocity at which oscillation of a liquid surface is suppressed in conveying a container in which a liquid is accommodated, e.g., a ladle in which molten metal is accommodated. In a graph of conveyance velocity versus conveyance time, an upwardly convex parabola and a downwardly convex parabola having vertical symmetry are prepared in advance, the downwardly convex parabola and the upwardly convex parabola are smoothly connected to form an acceleration curve, the upwardly convex parabola and the downwardly convex parabola are smoothly connected to form a deceleration curve, and the conveyance velocity is obtained from the acceleration curve and the deceleration curve smoothly connected where the slope thereof is zero.",
  "claims": [
    "1. A method for conveying a container, comprising: starting a conveyance by accelerating the container containing a liquid in a horizontal direction; and decelerating the container to complete the conveyance, wherein a conveyance velocity v(t) of the container, which is a function of time t, is represented by: Formula 1 when 0≤t≤(t 0 /4) v (t)= a·t 2 [Formula 1] Formula 2 when (t 0 /4)≤t≤(3t 0 /4) v ⁡ (t) = - a · [(t - t 0 2) 2 - t 0 2 8] [Formula ⁢ ⁢ 2] Formula 3 when (3t 0 /4)≤t≤(t 0) v (t)= a ·(t−t 0) 2 [Formula 3] wherein ‘t 0 ’ represents a time for conveying the container and ‘a’ represents a constant, and the method further comprises determining the conveyance velocity v(t) of the container by using Formulae 1 to 3, and driving a motor that rotates a plurality of wheels of a trolley on which the container is placed and conveying the container in accordance with the determined conveyance velocity v(t) such that liquid surface oscillations after conveying the container are within a tolerable range.",
    "2. The method for conveying a container according to claim 1, wherein: the conveyance velocity v(t) of the container, which is a function of time t, is also represented by: Formula 4 when 0≤t≤(t 1 /4) v (t)= b·t 2 [Formula 4] Formula 5 when (t 1 /4)≤t≤(t 1 /2) v ⁡ (t) = - b · [(t - t 1 2) 2 - t 1 2 8] [Formula ⁢ ⁢ 5] Formula 6 when (t 1 /2)≤t≤(t 1 /2)+t 2 v ⁡ (t) = 1 8 ⁢ b · t 1 2 [Formula ⁢ ⁢ 6] Formula 7 when (t 1 /2)+t 2 ≤t≤(3t 1 /4)+t 2 v ⁡ (t) = - b · [(t - t 1 2 - t 2) 2 - t 1 2 8] [Formula ⁢ ⁢ 7] Formula 8 when (3t 1 /4)+t 2 ≤t≤t 1 +t 2 v (t)= b ·(t−t 1 −t 2) 2 [Formula 8] wherein ‘t 1 ’ represents a total time for conveying the container in acceleration and in deceleration, ‘t 2 ’ represents a time for conveying the container at a constant speed, and ‘b’ represents a constant, and the method further comprises: setting the conveyance time v(t) of the container by using Formulae 1 to 3 when a maximum value of the conveyance velocity v(t) among Formulae 1 to 3 is equal to or less than a velocity limit V max for the container, which is tolerable in conveying the container; and setting the conveyance time v(t) of the container by using Formulae 4 to 8 and calculating the conveyance time t 1 and the conveyance time t 2 from the constant a, the velocity limit V max, and a conveyance distance L of the container where the constant b is equal to the constant a and the constant speed of Formula 6 is the velocity limit V max when the maximum value of the conveyance velocity v(t) among Formulae 1 to 3 is more than the velocity limit V max.",
    "3. The method for conveying a container according to claim 2, wherein the liquid is a molten metal and the container is a tilting ladle.",
    "4. The method for conveying a container according to claim 1, wherein the constant a is determined α max /2 wherein α max represents a maximum value of a rate of change of acceleration of the container at which liquid surface oscillations after conveying the container is suppressed within a tolerable range.",
    "5. The method for conveying a container according to claim 4, wherein a conveyance distance of the container is L and a velocity limit of the container that is tolerable in conveying the container is V max; the conveyance velocity v(t) of the container is set by Formulae 1 to 3 when a maximum value of the conveyance velocity v(t) among Formula 1 to 3 is equal to or less than the velocity limit V max; and when the maximum value of the conveyance velocity v(t) among Formulae 1 to 3 is more than the velocity limit V max, a total time for conveying the container in acceleration and in deceleration is t 1, a time for conveying the container at a constant speed is t 2, and the constant is b, and, in addition, the conveyance velocity v (t) of the container, which is a function of time t, is represented by: Formula 4 when 0≤t≤(t 1 /4) v (t)= b·t 2 [Formula 4] Formula 5 when (t 1 /4)≤t≤(t 1 /2) v ⁡ (t) = - b · [(t - t 1 2) 2 - t 1 2 8] [Formula ⁢ ⁢ 5] Formula 6 when (t 1 /2)≤t≤(t 1 /2)+t 2 v ⁡ (t) = 1 8 ⁢ b · t 1 2 [Formula ⁢ ⁢ 6] Formula 7 when (t 1 /2)+t 2 ≤t≤(3t 1 /4)+t 2 v ⁡ (t) = - b · [(t - t 1 2 - t 2) 2 - t 1 2 8] [Formula ⁢ ⁢ 7] Formula 8 when (3t 1 /4)+t 2 ≤t≤t 1 +t 2 v (t)= b ·(t−t 1 −t 2) 2 [Formula 8] wherein the conveyance velocity v(t) is set from the conveyance time t 1 and the conveyance time t 2 that are calculated from the constant a, the velocity limit V max, and the conveyance distance L where the constant b is the constant a and the constant speed of Formula 6 is the velocity limit V max.",
    "6. The method for conveying a container according to claim 1, wherein the liquid is a molten metal and the container is a tilting ladle.",
    "7. A conveyor control device for conveying a container, which starts conveying by accelerating the container containing a liquid in a horizontal direction and completes the conveyance after deceleration, the conveyor control device comprising: a computer, wherein the computer stores a conveyance time t 0 of the container, a constant a, a maximum value of a rate of change of acceleration of the container α max at which liquid surface oscillations after conveying the container are suppressed within a tolerable range; the computer also stores a conveyance velocity of the container v(t), which is a function of time t as: Formula 1 when 0≤t≤(t 0 /4) v (t)= a·t 2 [Formula 1] Formula 2 when (t 0 /4)≤t≤(3t 0 /4) v ⁡ (t) = - a · [(t - t 0 2) 2 - t 0 2 8] [Formula ⁢ ⁢ 2] Formula 3 when (3t 0 /4)≤t≤(t 0) v (t)= a ·(t−t 0) 2 [Formula 3] the computer is programmed to calculate the constant a from the stored rate of change of acceleration α max and determine the conveyance velocity v(t) of the container by using Formulae 1 to 3; and the computer is programmed to drive a motor that rotates a plurality of wheels of a trolley on which the container is placed and convey the container in accordance with the determined conveyance velocity v(t) such that the liquid surface oscillations after conveying the container are within the tolerable range.",
    "8. The conveyor control device unit for conveying a container according to claim 7, wherein the computer stores a conveyance distance L, a velocity limit V max for the container, which is tolerable in conveying the container, a total time t 1 for the container to be conveyed in acceleration and deceleration, a constant speed time t 2, and a constant b; the computer also stores the conveyance velocity of the container v(t), which is a function of time t as: Formula 4 when 0≤t≤(t 1 /4) v (t)= b·t 2 [Formula 4] Formula 5 when (t 1 /4)≤t≤(t 1 /2) v ⁡ (t) = - b · [(t - t 1 2) 2 - t 1 2 8] [Formula ⁢ ⁢ 5] Formula 6 when (t 1 /2)≤t≤(t 1 /2)+t 2 v ⁡ (t) = 1 8 ⁢ b · t 1 2 [Formula ⁢ ⁢ 6] Formula 7 when (t 1 /2)+t 2 ≤t≤(3t 1 /4)+t 2 v ⁡ (t) = - b · [(t - t 1 2 - t 2) 2 - t 1 2 8] [Formula ⁢ ⁢ 7] Formula 8 when (3t 1 /4)+t 2 ≤t≤t 1 +t 2 v (t)= b ·(t−t 1 −t 2) 2 [Formula 8] and when a maximum value of the conveyance velocity v(t) among Formulae 1 to 3 is equal to or less than the velocity limit V max, the computer is programmed to set the conveyance time v(t) of the container by using Formulae 1 to 3; and when the maximum value of the conveyance velocity v(t) among Formulae 1 to 3 is more than the velocity limit V max, the computer is programmed to set the conveyance time v(t) of the container by using Formulae 4 to 8, and, in addition, the computer is programmed to calculate the conveyance time t 1 and the conveyance time t 2 from the constant a, the velocity limit V max, and the conveyance distance L where the constant b is equal to the constant a and the constant speed of Formula 6 is the velocity limit V max."
  ],
  "description_excerpt": "The present invention relates to a method for conveying a container containing a liquid, and more particularly to a method for conveying a ladle containing molten metal.\n\nAn example of conveyance of a container containing a liquid is a conveyance of a ladle in a casting line. During this conveyance, after the ladle is conveyed to a pouring position, oscillations may be generated on a surface of molten metal in the ladle. If such oscillations continue for a long time, measurement of the ladle weight becomes unstable, which may affect feeding accuracy of the molten metal.\n\nIt has been known that such oscillations of a liquid surface can be suppressed by making a curve of acceleration and deceleration in a graph of velocity versus time of ladle conveyance an S shape. It has been also known that such an S-shaped curve can be calculated from a liquid simulation (Patent Document 1 for example).\n\nAs described in Patent Document 1, the calculation of the curve from a liquid simulation requires complex calculations using a plurality of parameters, such as conditions of the ladle and the molten metal, conveyance distance, conveyance time, and so on. However, it is often required in a casting line to change a ladle for another or to change the conveyance distance according to positions of molds. In such cases, it is required to change the above parameters according to the conditions and to do the complex calculations over again. That is, applying a liquid simulation to a conveyance of a ladle in a casting line may complicate setting of the conveyance velocity.",
  "cpc": [
    "B22D 41/12",
    "B22D 41/06",
    "B65B 57/00",
    "B65G 2813/023",
    "B65G 35/06",
    "B65G 43/00"
  ],
  "ipc": [
    "B22D 41/06",
    "B22D 41/12",
    "B65G 35/06",
    "B65G 43/00"
  ],
  "assignees": [
    "Hitachi Metals Ltd"
  ],
  "inventors": [
    "Takuya Harada"
  ],
  "filing_date": "2017-12-11",
  "publication_date": "2022-05-17",
  "grant_date": "2022-05-17",
  "priority_date": "2017-02-27",
  "application_number": "US-201716488412-A",
  "family_id": "63252541",
  "cited_by_count": 0,
  "citations": [
    "JPS51105017U",
    "US4491074A",
    "JPH0910924A",
    "JPH09277025A",
    "JP2006283786A",
    "US8062578B2",
    "WO2014174977A1",
    "US20170217695A1"
  ]
}

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