JPH02265614A - High gradient magnetic separation apparatus with continuously altering flow speed - Google Patents
High gradient magnetic separation apparatus with continuously altering flow speedInfo
- Publication number
- JPH02265614A JPH02265614A JP8537889A JP8537889A JPH02265614A JP H02265614 A JPH02265614 A JP H02265614A JP 8537889 A JP8537889 A JP 8537889A JP 8537889 A JP8537889 A JP 8537889A JP H02265614 A JPH02265614 A JP H02265614A
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- JP
- Japan
- Prior art keywords
- filter element
- shape
- gradient magnetic
- fluid
- magnetic separation
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Links
- 238000007885 magnetic separation Methods 0.000 title claims description 27
- 230000005291 magnetic effect Effects 0.000 claims abstract description 59
- 239000012530 fluid Substances 0.000 claims abstract description 38
- 239000010419 fine particle Substances 0.000 claims abstract description 19
- 239000003302 ferromagnetic material Substances 0.000 claims abstract description 5
- 239000000696 magnetic material Substances 0.000 claims abstract description 3
- 230000005294 ferromagnetic effect Effects 0.000 claims description 32
- 241000239290 Araneae Species 0.000 claims description 2
- 238000005530 etching Methods 0.000 claims description 2
- 238000004080 punching Methods 0.000 claims description 2
- 238000000034 method Methods 0.000 claims 1
- 239000000126 substance Substances 0.000 claims 1
- 239000006249 magnetic particle Substances 0.000 abstract description 6
- 238000001179 sorption measurement Methods 0.000 description 6
- 230000002093 peripheral effect Effects 0.000 description 5
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical compound [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 description 4
- 229910001220 stainless steel Inorganic materials 0.000 description 4
- XLYOFNOQVPJJNP-UHFFFAOYSA-N water Substances O XLYOFNOQVPJJNP-UHFFFAOYSA-N 0.000 description 4
- 230000004907 flux Effects 0.000 description 3
- 239000002245 particle Substances 0.000 description 3
- 230000007423 decrease Effects 0.000 description 2
- 229910052742 iron Inorganic materials 0.000 description 2
- 238000004519 manufacturing process Methods 0.000 description 2
- 238000000926 separation method Methods 0.000 description 2
- WLNBMPZUVDTASE-HXIISURNSA-N (2r,3r,4s,5r)-2-amino-3,4,5,6-tetrahydroxyhexanal;sulfuric acid Chemical compound [O-]S([O-])(=O)=O.O=C[C@H]([NH3+])[C@@H](O)[C@H](O)[C@H](O)CO.O=C[C@H]([NH3+])[C@@H](O)[C@H](O)[C@H](O)CO WLNBMPZUVDTASE-HXIISURNSA-N 0.000 description 1
- 239000004925 Acrylic resin Substances 0.000 description 1
- 229920000178 Acrylic resin Polymers 0.000 description 1
- 239000008280 blood Substances 0.000 description 1
- 210000004369 blood Anatomy 0.000 description 1
- 230000007797 corrosion Effects 0.000 description 1
- 238000005260 corrosion Methods 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000002474 experimental method Methods 0.000 description 1
- 230000005307 ferromagnetism Effects 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 239000012528 membrane Substances 0.000 description 1
- 239000007787 solid Substances 0.000 description 1
Landscapes
- Water Treatment By Electricity Or Magnetism (AREA)
Abstract
Description
【発明の詳細な説明】
(イ)産業上の利用分野
本発明は、流体中に含まれる磁性微粒子を効果的に捕集
することができる高勾配磁気分離装置に関する。DETAILED DESCRIPTION OF THE INVENTION (a) Field of Industrial Application The present invention relates to a high gradient magnetic separation device that can effectively collect magnetic particles contained in a fluid.
(ロ)従来の技術
従来、上記を目的とした高勾配磁気分離装置として特公
昭59−43208号公報に記載のものがある。(b) Prior Art Conventionally, there is a high gradient magnetic separation apparatus for the above purpose described in Japanese Patent Publication No. 59-43208.
第8図〜第1θ図にかかる高勾配磁気分離装置の内部構
造を示す。The internal structure of the high gradient magnetic separation apparatus according to FIGS. 8 to 1θ is shown.
図示するように、N!ff151とS磁8ii52との
間の空間に非磁性体セル53が配設されており、同非磁
性体セル53はその内部に微粒子を除去するためのフィ
ルタ空間を形成するとともに、その下部と上部に、それ
ぞれ、流入口54と流出口55とを設けている。As shown, N! A non-magnetic cell 53 is arranged in the space between the ff151 and the S magnet 8ii52. An inlet 54 and an outlet 55 are provided in each of the two.
また、非磁性体セル53内に形成したフィルタ空間には
、多数の強磁性細線56が処理流体の流れの方向と平行
に配設されている。Further, in the filter space formed within the non-magnetic cell 53, a large number of ferromagnetic thin wires 56 are arranged parallel to the flow direction of the processing fluid.
そして、これらの強磁性細線56は、等間隔を隔てて、
密で、しかも相互に平行に並設されている。These ferromagnetic thin wires 56 are arranged at equal intervals,
They are densely arranged and parallel to each other.
かかる構成によって、強磁性細線56を用いて周囲に高
勾配磁界を形成し、非常に小さい微粒子を吸着除去する
ことができる。With this configuration, a high gradient magnetic field is formed around the ferromagnetic thin wire 56, and very small particles can be adsorbed and removed.
ところで、上記高勾配磁気分離装置の性能は、一般に、
実効長さLeを用いて以下の式(1)で示される。By the way, the performance of the above-mentioned high gradient magnetic separation device is generally as follows.
It is expressed by the following equation (1) using the effective length Le.
Le−(L/a )(Vm/Vo ) ・ ・
・ (1)ここに、L、!=aはそれぞれ強磁性細線
の有効長と半径で、Voは処理水流速、V−は次式(2
)で与えられる磁気速度である。Le-(L/a)(Vm/Vo) ・ ・
・ (1) Here, L,! =a is the effective length and radius of the ferromagnetic thin wire, Vo is the flow rate of the treated water, and V- is the following formula (2
) is the magnetic velocity given by
V+*= (2/9 )(Zp ・MS−He・b
”/ 7/ ・a )・ ・ ・(2)
上記式(2)で、χ、とbは磁性微粒子の比磁化率と半
径、Msは強磁性III線の飽和磁束密度、■。V+*= (2/9) (Zp ・MS-He・b
”/ 7/ ・a)・・・・(2) In the above formula (2), χ and b are the relative magnetic susceptibility and radius of the magnetic fine particles, Ms is the saturation magnetic flux density of the ferromagnetic III wire, and ■.
は印加磁界の強さ、ηは微粒子に対する流体の粘性係数
である。is the strength of the applied magnetic field, and η is the viscosity coefficient of the fluid with respect to the particles.
つまり、Leの値が大きいほど高勾配磁気分離としての
性能は向上することになる。In other words, the larger the value of Le, the better the performance as high gradient magnetic separation.
(ハ)発明が解決しようとするm題
しかるにJ比磁化率のきわめて小さな微粒子を分離除去
するためには、(+)(2)式より、■極めて大きな磁
界勾配、したがって十分細い強磁性線を使用する必要が
あるが、かかる強磁性細線の製作は困難であり、また、
製造コストが高くなる。(c) Problem to be Solved by the Invention However, in order to separate and remove fine particles with an extremely small J-specific magnetic susceptibility, it is necessary to use (+) (2), an extremely large magnetic field gradient, and therefore a sufficiently thin ferromagnetic wire. However, it is difficult to produce such ferromagnetic thin wires, and
Manufacturing costs increase.
■印加磁界H0を大きく、或いは強磁性細線の有効長し
、即ち、フィルタの長さを長くする必要があるが、これ
らの要素を大きく、或いは長くすると、磁界発生装置が
非常に大きくなり、製造コストが高く迂る。■It is necessary to increase the applied magnetic field H0 or to increase the effective length of the ferromagnetic thin wire, that is, to increase the length of the filter, but if these elements are increased or lengthened, the magnetic field generator will become very large, making it difficult to manufacture. High cost and detour.
■処理水流速v0を低くする必要があるが、これは処理
水流速を低下させることにより、処理量が低下し、分離
除去装置としてのコストパフォーマンスが低くなる。(2) It is necessary to lower the flow rate v0 of the treated water, but this lowers the flow rate of the treated water, which lowers the throughput and lowers the cost performance of the separation and removal device.
本発明は、上記課題を解決することができる高勾配磁気
分離装置を提供することを目的とする。An object of the present invention is to provide a high gradient magnetic separation device that can solve the above problems.
(ニ)課題を解決するための手段
本発明は、処理流体の流路内に、強磁性体からなるフィ
ルタエレメントを配設して同流路内に磁場を形成し、同
強磁性体の周囲に形成される高勾配磁場により処理流体
中に浮遊する磁性微粒子を吸着除去させるための高勾配
磁気分離装置において、処理流体の流路の形状を、流路
の断面積が進行方向に漸次拡大するように形成し、フィ
ルタエレメントを通過する処理流体の流速が漸次低減さ
せるようにしたことを特徴とする高勾配磁気分離装置に
係るものである。(d) Means for Solving the Problems The present invention provides a filter element made of a ferromagnetic material in a flow path of a processing fluid, forms a magnetic field in the flow path, and creates a magnetic field around the ferromagnetic material. In a high-gradient magnetic separation device for adsorbing and removing magnetic fine particles suspended in a processing fluid using a high-gradient magnetic field formed in The present invention relates to a high gradient magnetic separation apparatus characterized in that the flow rate of the processing fluid passing through the filter element is gradually reduced.
また、上記構成においてフィルタエレメントの形状は、
■円柱状或いは円環や扇形等、円柱の一部を切り抜いた
形状、■球状或いは円錐や角錐等球の一部を切り抜いた
形状とすることができる。In addition, in the above configuration, the shape of the filter element is
(2) It can be cylindrical or a shape obtained by cutting out a part of a cylinder such as an annular shape or a sector; (2) It can be spherical or a shape obtained by cutting out a part of a sphere such as a cone or a pyramid.
さらに、上記■において、円柱状或いは円柱の一部を切
り抜いた形状をなすフィルタエレメントを構成する強磁
性細線が、円柱の径方向に沿って放射状に配置されてい
ること、及び■において、球状或いは球の一部を切り抜
いた形状をなすフィルタエレメントを構成する強磁性細
線が、球の径方向に沿って放射状に配置されていること
にも特徴を有する。Furthermore, in (1) above, the ferromagnetic thin wires constituting the filter element, which have a cylindrical shape or a shape obtained by cutting out a part of a cylinder, are arranged radially along the radial direction of the cylinder; Another feature is that the ferromagnetic thin wires constituting the filter element, which has a shape obtained by cutting out a part of a sphere, are arranged radially along the radial direction of the sphere.
(ホ)作用及び効果
本発明では、処理流体の波路の形状を、流路の断面積が
進行方向に漸次拡大するように形成し、フィルタエレメ
ントを通過する処理流体の流速が漸次低減させるように
したので、容易に発生しうる磁界強度及び従来の強磁性
ステンレス線を使用して比磁化率のきわめて小さな微粒
子を適量な処理量にて分離除去でき、小型で安価な高勾
配磁気分離装置を提供することができる。(E) Functions and Effects In the present invention, the shape of the wave path of the processing fluid is formed so that the cross-sectional area of the flow path gradually expands in the traveling direction, and the flow velocity of the processing fluid passing through the filter element is gradually reduced. Therefore, we provide a compact and inexpensive high-gradient magnetic separation device that can separate and remove fine particles with extremely low specific magnetic susceptibility at an appropriate throughput using easily generated magnetic field strength and conventional ferromagnetic stainless steel wire. can do.
(へ)実施例
以下、添付図に示す実施例に基づいて、本発明を具体的
に説明する。(f) Examples The present invention will be specifically described below based on examples shown in the attached drawings.
第1図〜第4図に、本実施例に係る高勾配磁気分離装置
Aの具体的構造を示す。1 to 4 show the specific structure of the high gradient magnetic separation apparatus A according to this embodiment.
第1図及び第2図において、10ば軟鉄等を素材とする
リターンフレームであり、後述する永久磁石11.12
とともに、磁気回路を形成することができる。In Figures 1 and 2, 10 is a return frame made of soft iron or the like, and permanent magnets 11 and 12, which will be described later, are used.
At the same time, a magnetic circuit can be formed.
本実施例において、かかるリターンフレーム10は、円
板状の上下壁10a、 lobと筒状の周壁10cとか
ら形成されている。In this embodiment, the return frame 10 is formed of disk-shaped upper and lower walls 10a and a lob, and a cylindrical peripheral wall 10c.
そして、リターンフレームIOは、その上下壁]Oa、
10bの内面に、それぞれ、ドーナノッ状の上下永久磁
石11.12を取付けており、両永久磁石II。Then, the return frame IO has its upper and lower walls ]Oa,
Upper and lower permanent magnets 11 and 12 in the form of dona knots are attached to the inner surface of 10b, respectively, and both permanent magnets II.
12の間の間隙に、後述する磁性微粒子20 (第5図
及び第6図参照)を吸着除去するための厚内円板状のフ
ィルタカートリッジ13を介設している。A filter cartridge 13 in the form of a thick inner disk is interposed in the gap between the filter cartridges 12 and 12 for adsorbing and removing magnetic fine particles 20 (see FIGS. 5 and 6), which will be described later.
また、リターンフレーム10の上壁10aの中央部に開
口14が設けられており、同開口14を上下方向に貫通
して流体流入管15が、リターンフレーム10の内部に
伸延しており、その伸延端に形成した開口部15aは、
フィルタカートリッジ13のL血中央部と連通連結して
いる。Further, an opening 14 is provided in the center of the upper wall 10a of the return frame 10, and a fluid inflow pipe 15 extends inside the return frame 10 by passing through the opening 14 in the vertical direction. The opening 15a formed at the end is
It is connected in communication with the central part of the L blood of the filter cartridge 13.
一方、フィルタカートリッジ13の周壁部には複数の流
体流出管16が連通連結されている。On the other hand, a plurality of fluid outflow pipes 16 are connected to the peripheral wall of the filter cartridge 13 .
本発明は8.実質的に、上記フィルタカートリッジ13
の内部構成に要旨を有する。The present invention is 8. Substantially, the filter cartridge 13
The gist is in the internal structure of.
即ち、本実施例において、かかるフィルタカートリッジ
13は、第1図に示すように、薄肉円板状の上下壁と薄
肉周壁とからなる中空筒状フィルタ容器17と、同中空
筒状フィルタ 容器17内に積層状態に配設した多数の
円盤状のフィルタエレメント(又はフィルタモジュール
)18とからなる。That is, in this embodiment, as shown in FIG. 1, the filter cartridge 13 includes a hollow cylindrical filter container 17 made up of thin disc-shaped upper and lower walls and a thin peripheral wall, and a hollow cylindrical filter container 17 that includes a hollow cylindrical filter container 17 that includes thin disc-shaped upper and lower walls and a thin peripheral wall. It consists of a large number of disc-shaped filter elements (or filter modules) 18 arranged in a stacked manner.
そして、各フィルタエレメント18は、第3図、第4図
及び第5図に示すように、多数の強磁性細線19を36
0″全方向に放射状に配設しており、強磁性細線19間
に形成される流路Pの断面積が、フィルタエレメント1
8の中央部から外周縁に向かって漸次太き(なるように
している。As shown in FIGS. 3, 4, and 5, each filter element 18 includes a large number of ferromagnetic thin wires 19 at 36.
0'' are arranged radially in all directions, and the cross-sectional area of the flow path P formed between the ferromagnetic thin wires 19 is the same as that of the filter element 1.
It gradually becomes thicker from the center of 8 toward the outer periphery.
かかる構成によって、各フィルタエレメント18に流入
した処理流体の速度は、フィルタエレメント18の中央
部から外周縁に向かって流れるにつれて漸次遅くなるこ
とになる。With this configuration, the speed of the processing fluid flowing into each filter element 18 becomes gradually slower as it flows from the center of the filter element 18 toward the outer periphery.
つまり、フィルタカートリッジ13における処理水の流
れにおいて、放射状に強磁性細線19を配置した各フィ
ルタニレメン目8の任意における流速は常に変化し、中
心部近傍の流速に比べて外周近傍の流速は半径に反比例
して低下することになる。In other words, in the flow of treated water in the filter cartridge 13, the flow velocity at any point in each filter element 8 in which the ferromagnetic thin wires 19 are arranged radially changes, and the flow velocity near the outer periphery is lower than the flow velocity near the center. will decrease in inverse proportion to.
ただし、径方向に対して、フィルタエレメント18の単
位体積当たりの強磁性細線19の空間占積率を略同−に
するために、強磁性細線19は多段階に放射状に配置し
ている。即ち、強磁性細線19の単位中心各当たりの密
度は、中央部は粗に、外周縁に向かうに従って漸次密に
配置している。However, in order to make the space factor of the ferromagnetic wires 19 per unit volume of the filter element 18 substantially the same in the radial direction, the ferromagnetic wires 19 are arranged radially in multiple stages. That is, the density per unit center of the ferromagnetic thin wires 19 is coarse in the center and gradually denser toward the outer periphery.
次に、上記構成を有する本発明に係る高勾配磁気分離装
置Aの微粒子吸着除去原理を、従来装置の場合と比較し
ながら、第5図及び第6図を参照し゛ζ説明する。Next, the principle of adsorption and removal of particulates in the high gradient magnetic separation apparatus A according to the present invention having the above configuration will be explained with reference to FIGS. 5 and 6, while comparing it with the conventional apparatus.
第5図(X−Z断面図)において、磁界はX方向に印加
されており、磁性微粒子20を含んだ処理流体はY方向
へ流れる。(つまり紙面の裏から表へ流れている。)
そして、第5図において、強磁性細線19の近傍には磁
界の歪みが生じて、処理流体中に浮遊する磁性微粒子2
0に磁気吸引力が働き、実線矢印で示した様な軌跡に沿
って磁性微粒子20は移動し、最終的に磁性線19に吸
着されることになる。In FIG. 5 (X-Z sectional view), the magnetic field is applied in the X direction, and the processing fluid containing the magnetic particles 20 flows in the Y direction. (In other words, it flows from the back to the front of the paper.) In FIG. 5, a distortion of the magnetic field occurs near the ferromagnetic wire 19, and the magnetic fine particles 2 floating in the processing fluid
A magnetic attraction force acts on the magnetic particles 20, and the magnetic fine particles 20 move along the trajectory shown by the solid arrow, and are finally attracted to the magnetic wire 19.
即ち、X−Z断面における磁性微粒子20の吸着軌跡は
、本発明も従来技術においても違いが生じない。That is, there is no difference in the adsorption trajectory of the magnetic fine particles 20 in the X-Z cross section between the present invention and the prior art.
次にX−Z断面における磁性微粒子20が強磁性細線1
9に吸着されるまでの軌跡を第6図に示す。Next, the magnetic fine particles 20 in the X-Z cross section are the ferromagnetic thin wires 1.
Fig. 6 shows the trajectory until it is adsorbed by 9.
この場合、処理流体の流れの方向は紙面の上から下へと
流れていることになる。In this case, the flow direction of the processing fluid is from the top to the bottom of the page.
従来技術における磁性微粒子20の軌跡は一点鎖線で示
し、本発明における磁性微粒子20の軌跡は破線で示す
。The locus of the magnetic fine particles 20 in the prior art is shown by a dashed line, and the locus of the magnetic fine particles 20 in the present invention is shown by a broken line.
図示するように、本発明と従来技術との間には明らかな
相違があり、磁性微粒子20を強磁性細線19に吸着す
るまでの本発明による有効磁性線長さ21が従来技術に
よる有効磁性線長さ2.に比べてかなり短くなっている
ことがわかる。As shown in the figure, there is a clear difference between the present invention and the prior art, and the effective magnetic line length 21 according to the present invention until the magnetic fine particles 20 are attracted to the ferromagnetic thin wire 19 is different from the effective magnetic line length 21 according to the prior art. Length 2. It can be seen that it is considerably shorter than .
つまり、処理流体の初期流速が同じである場合、従来技
術では流速が各フィルタエレメント18の中央部側の流
入口から外周縁側の流出口まで、すべての位置で一定で
ある。In other words, when the initial flow velocity of the processing fluid is the same, in the prior art, the flow velocity is constant at all positions from the inlet on the center side of each filter element 18 to the outlet on the outer peripheral edge side.
これに対して、本発明では、任意の位置の流速が、初期
流速に対して、フィルタエレメント18の中央部側の流
入口から処理流体が進んだ距離に対して反比例的に低下
するため、強磁性細線19の有効長さが短い場所にて磁
性微粒子20を吸着可能となる。In contrast, in the present invention, the flow velocity at any position decreases inversely proportional to the distance traveled by the processing fluid from the inlet on the center side of the filter element 18 with respect to the initial flow velocity. The magnetic fine particles 20 can be attracted at a location where the effective length of the magnetic thin wire 19 is short.
従って、本発明による磁性微粒子吸着除去範囲帽は、従
来技術による磁性微粒子吸着除去範囲1に比べて、磁性
線19の一本当たりの微粒子吸着除去範囲を、第6図に
二点鎖線で示すように、大幅に向上することができる。Therefore, the magnetic particulate adsorption/removal range cap according to the present invention has a particulate adsorption/removal range per magnetic wire 19 as shown by the two-dot chain line in FIG. can be significantly improved.
なお、上記した実施例においては、磁場を形成するため
、永久磁石11.12を用いたが、これに限定されるも
のではな(、電磁石、超電導磁石等により磁場を形成す
ることもできる。In the above-described embodiment, permanent magnets 11 and 12 were used to form a magnetic field, but the present invention is not limited thereto (the magnetic field may also be formed using an electromagnet, a superconducting magnet, etc.).
また、強磁性細線19は、腐食等を考慮して、強磁性の
ステンレス線を用いるのが好ましいが、何らステンレス
線に限定されるものではなく、強磁性を有するものであ
れば、他の素材からなる線を用いることもできる。In addition, it is preferable to use a ferromagnetic stainless steel wire as the ferromagnetic thin wire 19 in consideration of corrosion etc. However, it is not limited to stainless steel wire in any way, and may be made of other materials as long as it has ferromagnetism. It is also possible to use a line consisting of
また、強磁性細線磁性線19によって形成されるフィル
タエレメント18の形状は、■円柱状或いは円環や扇形
等、円柱の一部を切り抜いた形状、■球状或いは円錐や
角錐等球の一部を切り抜いた形状とすることができる。In addition, the shape of the filter element 18 formed by the ferromagnetic thin magnetic wire 19 is: (1) cylindrical shape or a shape in which a part of a cylinder is cut out, such as an annular shape or a fan shape; (2) a spherical shape or a shape in which a part of a sphere such as a cone or a pyramid is It can be cut out.
さらに、上記のにおいて、フィルタエレメント18を形
成する強磁性細線19を、円柱の径方向に沿って放射状
に配置したり、■において、フィルタエレメント1Bを
構成する強磁性細線19を、球の径方向に沿って放射状
に配置するようにすることもできる。 [
以下、第1図〜第3図に示す構造を有する高勾配磁気分
離袋WLAを実際に製作し、実験を行った。Furthermore, in the above, the ferromagnetic thin wires 19 forming the filter element 18 are arranged radially along the radial direction of the cylinder, and in They can also be arranged radially along. [Hereinafter, a high gradient magnetic separation bag WLA having the structure shown in FIGS. 1 to 3 was actually manufactured and an experiment was conducted.
まず、同装置Aの具体的構成及び諸元等について説明す
る。First, the specific configuration and specifications of the device A will be explained.
円盤状軸方向に着磁された永久磁石11.12(Nd−
Pa−B系、残留磁束密度Br−12,000(G)、
保磁力Hc−11、000(Oe) 、エネルギ積(B
−[1)wax =35(MGOe))を、第1図に示
すように異極を空隙3抛−で対面させ、その周囲を軟鉄
を素材とするリターンフレーム10で囲み、磁気回路を
構成した。Permanent magnet 11.12 (Nd-
Pa-B system, residual magnetic flux density Br-12,000 (G),
Coercive force Hc-11,000 (Oe), energy product (B
- [1) wax = 35 (MGOe)), as shown in Fig. 1, the different poles are faced with three air gaps, and the periphery is surrounded by a return frame 10 made of soft iron to form a magnetic circuit. .
その時に永久磁石11.12間の間隙部において発生す
る磁界強度は、約5,500Gであった。At that time, the magnetic field strength generated in the gap between the permanent magnets 11 and 12 was about 5,500G.
その空隙部に非磁性体であるアクリル樹脂によって製作
したフィルタ容器17を配置し、同フィルタ容器17内
に、第4図に示すようなフィルタニレメン)18を25
枚積層状態に組み込み、フィルタエレメント18を形成
した。A filter container 17 made of acrylic resin, which is a non-magnetic material, is placed in the gap, and inside the filter container 17, 25 filter membranes 18 as shown in FIG. 4 are placed.
The filter elements 18 were assembled in a laminated state.
各フィルタエレメント18の形状・寸法は、最外径−2
00鴎φ、最内径−20■φとし、その間の第1段目の
外径−80−φ、第2段目の外径−140mφ、第3段
目の外径−最外径となるように3段配置とした。The shape and dimensions of each filter element 18 are the outermost diameter -2
00mmφ, innermost diameter -20mmφ, and between them, the outer diameter of the first stage is -80mmφ, the outer diameter of the second stage is -140mφ, and the outer diameter of the third stage is - the outermost diameter. It was arranged in three stages.
それぞれの各段には、外径100 /711φのフェラ
イト系ステンレス鋼からなり、飽和磁束密度Ms(−1
,77)の強磁性細線19を、空間占積率6%にして放
射状に配列した。Each stage is made of ferritic stainless steel with an outer diameter of 100/711φ and has a saturation magnetic flux density Ms (-1
, 77) were arranged radially with a space factor of 6%.
流体流入口15はリターンフレーム10の上面中央部に
設けるとともに、流体流出口16はリターンフレーム1
0の周面に、円周方向に30°間隔あけて12個設けた
。The fluid inlet 15 is provided at the center of the upper surface of the return frame 10, and the fluid outlet 16 is provided at the center of the upper surface of the return frame 10.
Twelve pieces were provided on the circumferential surface of 0 at intervals of 30° in the circumferential direction.
かかる構成によって、処理流体は、流体流入口15より
フィルタカートリッジ13のフィルタエレメント18内
に流入し、多数のフィルタエレメント18が設置されて
いるフィルタ容器17内を、中央部から外周部に向けて
流れ、流体流出口16より流出されることになる。With this configuration, the processing fluid flows into the filter element 18 of the filter cartridge 13 from the fluid inlet 15, and flows from the center toward the outer periphery within the filter container 17 in which a large number of filter elements 18 are installed. , the fluid is discharged from the fluid outlet 16.
平均粒径lμ−のα−Pe203の磁性微粒子19が濃
度としてl(1+g/j!で懸濁している非処理流体を
、処理流量を変えて、上記した高勾配磁気分離装置Aで
処理した場合の微粒子除去機能を、以下の第1表に示す
。When an untreated fluid in which magnetic fine particles 19 of α-Pe203 with an average particle diameter of lμ− are suspended at a concentration of l(1+g/j!) is treated with the above-mentioned high gradient magnetic separation device A by changing the treatment flow rate. The particulate removal function of is shown in Table 1 below.
第1表(磁性微粒子分離除去性能)
第1表からも明らかなように、本発明に係る高勾配磁気
分離装置Aは、磁性微粒子17を、広流量範囲にわたっ
て、高効率(85〜97%)で吸着除去できる。Table 1 (Magnetic fine particle separation and removal performance) As is clear from Table 1, the high gradient magnetic separation apparatus A according to the present invention can separate magnetic fine particles 17 with high efficiency (85 to 97%) over a wide flow rate range. It can be removed by adsorption.
尚、磁気分離装置Aのフィルタエレメントを構成する強
磁性細線は、強磁性体の薄板をエツチングまたは、打ち
抜き等により細線部分が残るように加工したもの又は、
非磁性体薄板に、強磁性体をプリント加工したものでも
よい。また、磁性細線を投網状或いは、蜘蛛の巣状に編
んだ網でもよい。The ferromagnetic fine wires constituting the filter element of the magnetic separation device A are those obtained by etching or punching a thin ferromagnetic plate so that a thin wire portion remains, or
A ferromagnetic material may be printed on a non-magnetic thin plate. Alternatively, it may be a net made of magnetic fine wires woven into a cast net shape or a spider web shape.
第1図は本発明に係る高勾配磁気分離装置の断面正面図
、第2図は同平面図、第3図は第1図I−1線による横
断面図、第4図はフィルタエレメントの斜視図、第5図
はフィルタエレメントの一部拡大斜視図、第6図及び第
7図は磁性微粒子の吸着原理説明図、第8図は従来の高
勾配磁気分離装置の概念的構成を示す斜視図、第9図は
同断面側面図、第1O図は第9図■−■線による横断面
図である。
図中、
A:高勾配磁気分離装置
P:流路
10: リターンフレーム
11:永久磁石
12:永久磁石
13: フィルタカートリッジ
14;開口
15:流体流入管
16:流体流出管
17:中空筒状フィルタ容器
18: フィルタエレメント
19:強磁性細線
20:磁性微粒子Fig. 1 is a cross-sectional front view of a high gradient magnetic separation device according to the present invention, Fig. 2 is a plan view thereof, Fig. 3 is a cross-sectional view taken along line I-1 in Fig. 1, and Fig. 4 is a perspective view of a filter element. Figure 5 is a partially enlarged perspective view of the filter element, Figures 6 and 7 are diagrams explaining the principle of adsorption of magnetic particles, and Figure 8 is a perspective view showing the conceptual configuration of a conventional high gradient magnetic separation device. , FIG. 9 is a cross-sectional side view of the same, and FIG. 1O is a cross-sectional view taken along the line ■-■ in FIG. In the figure, A: High gradient magnetic separation device P: Channel 10: Return frame 11: Permanent magnet 12: Permanent magnet 13: Filter cartridge 14; Opening 15: Fluid inflow pipe 16: Fluid outflow pipe 17: Hollow cylindrical filter container 18: Filter element 19: Ferromagnetic thin wire 20: Magnetic fine particles
Claims (1)
レメントを配設して同流路内に磁場を形成し、同磁性体
の周囲に形成される高勾配磁場により処理流体中に浮遊
する磁性微粒子を吸着除去させるための高勾配磁気分離
装置において、処理流体の流路の形状を、流路の断面積
が進行方向に漸次拡大するように形成し、フィルタエレ
メントを通過する処理流体の流速が漸次低減させるよう
にしたことを特徴とする流速が連続的に変化する高勾配
磁気分離装置。 2、フィルタエレメントの形状が、円柱状或いは円環や
扇形等、円柱の一部を切り抜いた形状をなしていること
を特徴とする請求項1記載の流速が連続的に変化する高
勾配磁気分離装置。 3、フィルタエレメントの形状が、球状或いは円錐や角
錐等球の一部を切り抜いた形状をなしていることを特徴
とする流速が連続的に変化する請求項1記載の高勾配磁
気分離装置。 4、円柱状或いは円柱の一部を切り抜いた形状をなすフ
ィルタエレメントを構成する強磁性細線が、円柱の径方
向に沿って放射状に配置されていることを特徴とする流
速が連続的に変化する請求項2記載の高勾配磁気分離装
置。 5、球状或いは球の一部を切り抜いた形状をなすフィル
タエレメントを構成する強磁性細線が、球の径方向に沿
って放射状に配置されていることを特徴とする流速が連
続的に変化する請求項3記載の高勾配磁気分離装置。 6、強磁性細線を放射状に配置したフィルタエレメント
が強磁性体の薄板をエッチング又は打ち抜き加工により
細線部が残るように加工したもの、又は、非磁性体薄板
に強磁性体をプリント加工したものからなることを特徴
とする流速が連続的に変化する請求項4項記載の高勾配
磁気分離装置。 7、磁性体細線を放射状に配置したフィルタエレメント
が、磁性細線を投網状、或いは蜘蛛の巣状に編んだ網か
らなることを特徴とする流速が連続的に変化する請求項
4項記載の高勾配磁気分離装置。[Claims] 1. A filter element made of a ferromagnetic material is disposed in the flow path of the processing fluid to form a magnetic field in the flow path, and a high gradient magnetic field is formed around the magnetic material. In a high-gradient magnetic separation device for adsorbing and removing magnetic fine particles suspended in a processing fluid, the shape of the flow path of the processing fluid is formed so that the cross-sectional area of the flow path gradually expands in the direction of movement, and the filter element A high-gradient magnetic separation device in which the flow rate changes continuously, characterized in that the flow rate of a processing fluid passing through the process fluid is gradually reduced. 2. The high-gradient magnetic separation in which the flow rate changes continuously according to claim 1, wherein the filter element has a shape such as a cylinder, or a shape obtained by cutting out a part of a cylinder, such as an annular shape or a fan shape. Device. 3. The high-gradient magnetic separation apparatus according to claim 1, wherein the filter element has a shape that is spherical or a shape obtained by cutting out a part of a sphere such as a cone or a pyramid, and the flow velocity changes continuously. 4. The ferromagnetic thin wires constituting the filter element, which has a cylindrical shape or a shape obtained by cutting out a part of a cylinder, are arranged radially along the radial direction of the cylinder.The flow velocity changes continuously. The high gradient magnetic separation apparatus according to claim 2. 5. A claim in which the flow velocity changes continuously, characterized in that the ferromagnetic thin wires constituting the filter element, which are spherical or have a shape obtained by cutting out a part of a sphere, are arranged radially along the radial direction of the sphere. Item 3. High gradient magnetic separation device. 6. The filter element, in which fine ferromagnetic wires are arranged radially, is made by etching or punching a thin ferromagnetic plate so that the fine wire portion remains, or by printing a ferromagnetic substance on a thin non-magnetic plate. 5. The high gradient magnetic separation apparatus according to claim 4, wherein the flow rate changes continuously. 7. The filter element according to claim 4, wherein the filter element in which the magnetic thin wires are arranged radially is made of a mesh of magnetic thin wires woven in a cast net shape or a spider web shape, and the flow velocity changes continuously. Gradient magnetic separation device.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP8537889A JPH02265614A (en) | 1989-04-03 | 1989-04-03 | High gradient magnetic separation apparatus with continuously altering flow speed |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP8537889A JPH02265614A (en) | 1989-04-03 | 1989-04-03 | High gradient magnetic separation apparatus with continuously altering flow speed |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH02265614A true JPH02265614A (en) | 1990-10-30 |
Family
ID=13857066
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP8537889A Pending JPH02265614A (en) | 1989-04-03 | 1989-04-03 | High gradient magnetic separation apparatus with continuously altering flow speed |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH02265614A (en) |
Citations (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5143208A (en) * | 1974-10-04 | 1976-04-13 | Ssp Agric Equip | SOFUKI |
| JPS5514707B2 (en) * | 1976-07-10 | 1980-04-18 | ||
| JPS5676215A (en) * | 1979-11-26 | 1981-06-23 | Hitachi Plant Eng & Constr Co Ltd | Magnetic filter |
| JPS6159163A (en) * | 1984-08-30 | 1986-03-26 | 松下電器産業株式会社 | Controller for quantity of refrigerant circulated in refrigerant heating type air conditioner |
| JPS62204819A (en) * | 1986-03-06 | 1987-09-09 | Daido Steel Co Ltd | Multi-flow velocity magnetic filter |
| JPS63315115A (en) * | 1987-06-15 | 1988-12-22 | Nippon Steel Corp | Removing method for magnetic particle subjected to magnetic separation |
-
1989
- 1989-04-03 JP JP8537889A patent/JPH02265614A/en active Pending
Patent Citations (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5143208A (en) * | 1974-10-04 | 1976-04-13 | Ssp Agric Equip | SOFUKI |
| JPS5514707B2 (en) * | 1976-07-10 | 1980-04-18 | ||
| JPS5676215A (en) * | 1979-11-26 | 1981-06-23 | Hitachi Plant Eng & Constr Co Ltd | Magnetic filter |
| JPS6159163A (en) * | 1984-08-30 | 1986-03-26 | 松下電器産業株式会社 | Controller for quantity of refrigerant circulated in refrigerant heating type air conditioner |
| JPS62204819A (en) * | 1986-03-06 | 1987-09-09 | Daido Steel Co Ltd | Multi-flow velocity magnetic filter |
| JPS63315115A (en) * | 1987-06-15 | 1988-12-22 | Nippon Steel Corp | Removing method for magnetic particle subjected to magnetic separation |
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