Method of an apparatus for sifting particulate material in a cross-current

Claim 2

In apparatus for sifting particulate material in a cross-current comprising: (a) a flow duct for material charged sifting gas having an inlet opening and a material charging opening essentially perpendicular thereto; (b) means supplying a sifting gas current at high velocity to said inlet opening; (c) means for propelling material to be separated to a charging point at said charging opening in said duct and into said sifting zone, said means arranged to propel said material transversely with respect to the sifting gas current; (d) at least one knife edge pointed so as to oppose the trajectory of the material propelled into said sifting zone; (e) a coarse material collecting receptacle on the side of said knife edge opposite the material charging point; and (f) a discharge duct on the other side of said knife edge, wherein the improvement comprises: (g) an additional discharge duct having an inlet opening into said sifting zone duct down stream of the material charging point and immediately therebehind for drawing a partial current of the entering sifting gas therethrough, said duct extending primarily in a direction opposite said material input direction such as to have its current component with a direction opposite the material input direction.

Claim 3

Apparatus according to claim 1 and further including an adjustable knife edge blade disposed at said additional discharge duct inlet opening.

Claim 4

Apparatus according to claim 1 wherein said sifting flow duct is of a rectangular construction and wherein said means for propelling said material into said sifting gas comprises a conveyor belt and further including means rotating at the same speed as said conveyor belt disposed thereabove at the material charging point.

Claim 5

Apparatus according to claim 3 wherein said means rotating comprise and additional conveyor belt.

Claim 6

Apparatus according to claim 3 wherein said means rotating comprise a roller.

Claim 7

Apparatus according to claim 1 wherein said means for charging material into said sifting zone comprise a pneumatic charging device.

Claim 8

Apparatus according to claim 1 wherein said sifting zone duct is a symmetrical flow duct having an annular inlet opening and wherein said means for charging material into said sifting zone comprise a centrifugal plate coaxial with said inlet opening, said plate having an external diameter which is not larger than the internal diameter of said flow duct.

Claim 9

Apparatus according to claim 7 wherein said centrifugal plate has a wall which is contacted by the material to be sifted in the form of a concave curved rotational surface at least in its outer radial region and further including a cover extending a least slight distance to the outer edge of said plate.

Claim 10

Apparatus according to claim 1 and further including a top depression associated with said coarse material collecting receptacle and an obliquely downward directed wall associated therewith to cause material carried upwardly by a rotating secondary gas current to be returned into the coarse material collecting receptacle.

Claim 11

Apparatus according to claim 1 wherein said knife edge and adjustable knife edge blade and the walls defining said coarse material receptacle, said flow duct and said discharge duct are inclined toward the trajectories such that material trajectories encountering said knife edges and walls along with any reflecged trajectories therefrom are always directed into the interior of said receptacle and ducts even in the case of a vertical rebound.

Claim 12

In a method for sifting particulate material in a cross current comprising the steps of: (a) establishing a high velocity sifting gas current; (b) propelling the particles to be sifted into the sifting gas current at a separating zone with all the particles of the same size having the same velocity of at least approximately 5m/sec at a material charging point in a thin layer transverse to the direction of the sifting gas current whereby said particles will be spread out according to size based on their individual momentum and the current of the sifting gas; (c) after a time of flight of the order of magnitude of 1/100 sec. separating the spread out particles into at least two fractions using one or more knife edges pointing in a direction opposite to the trajectories of the material, and separation being carried out without any material previously rebounding from any wall; and (d) subdividing the incoming sifting gas current into at least two parts and leading off said parts separately, the improvement comprising: (e) drawing off a partial current directly after the material charging point in a direction different from the influx direction of the sifting gas current said partial current having a current momentum component in a direction opposite to the direction in which the material is propelled into the sifting gas current which has a value which is at least 1/10 of that of the momentum of the momentum of the current of material being propelled into the sifting gas, whereby said partial current will have a stabilizing effect on the separation with varying throughputs of the material.

Claim 13

In a method for sifting particulate material in a cross current comprising the steps of: (a) establishing a high velocity sifting gas current; (b) propelling the particles to be sifted into the sifting gas current at a separating zone with all the particles of the same size having the same velocity of at least approximately 5m/sec at a material charging point in a thin layer transverse to the direction of the sifting gas current whereby said particles will be spread out according to size based on their individual momentum and the current of the sifting gas; (c) after a time of flight of the order of magnitude of 1/100 sec. separating the spread out particles into at least two fractions using one or more knife edges pointing in a direction opposite to the trajectories of the material, and separation being carried out without any material previously rebounding from any wall; and (d) subdividing the incoming sifting gas current into at least two parts and leading off said parts separately, the improvement comprising: (e) drawing off a partial current directly after the material charging point in a direction different from the influx direction of the sifting gas current said partial current having a current momentum component in a direction opposite to the direction in which the material is propelled into the sifting gas current which has a value which is at least 1/10 of that of the momentum of the momentum of the current of material being propelled into the sifting gas, whereby said partial current will have a stabilizing effect on the separation with varying throughputs of the material.

Claim 14

The method according to claim 11 wherein the at least two fractions include a coarse fraction and a middle fraction and wherein a finest fraction is carried off by said partial current.

Claim 15

The method according to claim 11 and further including the step of introducing a portion of the oncoming sifting gas along with said material into the separating zone.

Claim 16

The method according to claim 11 wherein said sifting gas current is rotationally symmetric and further including the step of providing said sifting gas current with a rotational component.

Claim 17

The method according to claim 11 wherein one of the fractions into which the incoming sifting gas current is subdivided carries therewith a middle fraction of the material being separated and wherein said fraction is at least partially recharged into the sifting zone at least partially with the material to be sifted.

Claim 18

The method according to claim 11 wherein one of said parts which are led off separately is led off with the coarse material and wherein said part is a small part of less than 10% of the incoming sifting gas current.

Claim 19

The method according to claim 11 and further including the step of varying the quantity of sifting gas partial current drawn off as a function of the mass current of the charged material such that the mass current ratio of the two fractions of material one remains constant or assumes a predetermined value dependent on the absolute valve of the mass current so as to control the action in the separating zone.

Claim 20

In a method for sifting particulate material in a cross current comprising the steps of: (a) establishing a high velocity sifting gas current; (b) propelling the particles to be sifted into the sifting gas current at a separating zone with all the particles of the same size having the same velocity of at least approximately 5m/sec at a material charging point in a thin layer transverse to the direction of the sifting gas current whereby said particles will spread out according to size based on their individual momentum and the current of the sifting gas; (c) after a time of flight of the order of magnitude of 1/100 sec. separating the spread out particles into at least two fractions using one or more knife edges pointing in a direction opposite to the trajectories of the material, said separation being carried out without any material previously rebounding from any wall; and (d) subidviding the incoming sifting gas current into at least two parts and leading off said parts separately, the improvement comprising: (e) drawing off a partial current directly after the material charging point in a direction different from the influx direction of the sifting gas current said partial current having a current momentum in a directin opposite to the direction in which the material is propelled into the sifting gas current which has a value which is of the same order of magnitude as the momentum of the current of material being propelled into the sifting gas.

Claim 21

In a method for sifting particulate material in a cross current comprising the steps of: (a) establishing a high velocity sifting gas current; (b) propelling the particles to be sifted into the sifting gas current at a separating zone with all the particles of the same size having the same velocity of at least approximately 5m/sec at a material charging point in a thin layer transverse to the direction of the sifting gas current whereby said particles will spread out according to size based on their individual momentum and the current of the sifting gas; (c) after a time of flight of the order of magnitude of 1/100 sec. separating the spread out particles into at least two fractions using one or more knife edges pointing in a direction opposite to the trajectories of the material, said separation being carried out without any material previously rebounding from any wall; and (d) subidviding the incoming sifting gas current into at least two parts and leading off said parts separately, the improvement comprising: (e) drawing off a partial current directly after the material charging point in a direction different from the influx direction of the sifting gas current said partial current having a current momentum in a directin opposite to the direction in which the material is propelled into the sifting gas current which has a value which is of the same order of magnitude as the momentum of the current of material being propelled into the sifting gas.

Claim 22

In a method for siftingg particulate material in a cross current comprising the steps of: (a) establishing a high velocity sifting gas current; (b) propelling the particles to be sifted into the sifting gas current at a separating zone with all the particles of the same size having the same velocity of at least approximately 5m/sec at a material charging point in a thin layer transverse to the direction of the sifting gas current whereby said particles will spread out according to size based on their individual momentum and the current of the sifting gas; (c) after a time of flight of the order of magnitude of 1/100 sec. separating the spread out particles into at least two fractions using one or more knife edges pointing in a direction opposite to the trajectories of the material, said separation being carried out without any material previously rebounding from any wall; and (d) subdividing the incoming sifting gas current into at least two parts and leading off said parts separately, the improvement comrising: (e) drawing off a partial current directly after the material chrging point in a direction different from the influx direction of the sifting gas current said partial current having a current momentum component in a direction opposite to the direction in which the material is propelled into the sifting gas current which has a value which is at least 1/10 of that of sifting gas; and (f) adjusting the partial current velocity component v which is in a direction opposite to the material input direct, the material input velocity w and the aperture width s of the partial current which is drawn off so as to approximately satisfy the condition. s. v/w ≧ 1 mm.

Claim 23

In a method for siftingg particulate material in a cross current comprising the steps of: (a) establishing a high velocity sifting gas current; (b) propelling the particles to be sifted into the sifting gas current at a separating zone with all the particles of the same size having the same velocity of at least approximately 5m/sec at a material charging point in a thin layer transverse to the direction of the sifting gas current whereby said particles will spread out according to size based on their individual momentum and the current of the sifting gas; (c) after a time of flight of the order of magnitude of 1/100 sec. separating the spread out particles into at least two fractions using one or more knife edges pointing in a direction opposite to the trajectories of the material, said separation being carried out without any material previously rebounding from any wall; and (d) subdividing the incoming sifting gas current into at least two parts and leading off said parts separately, the improvement comrising: (e) drawing off a partial current directly after the material chrging point in a direction different from the influx direction of the sifting gas current said partial current having a current momentum component in a direction opposite to the direction in which the material is propelled into the sifting gas current which has a value which is at least 1/10 of that of sifting gas; and (f) adjusting the partial current velocity component v which is in a direction opposite to the material input direct, the material input velocity w and the aperture width s of the partial current which is drawn off so as to approximately satisfy the condition. s. v/w ≧ 1 mm.

Claim 24

In a method for sifting particulate material in a cross current comprising the steps of: (a) establishing a high velocity sifting gas current; (b) propelling the particles to be sifted into the sifting gas current at a separating zone with all the particles of the same size having the same velocity of at least approximately 5 m/sec at a material charging point in a thin layer transverse to the direction of the sifting gas current whereby said particles will spread out according to size based on their individual momentum and the current of the sifting gas; (c) after a time of flight of the order of magnitude of 1/100 sec. separating the spread out particles into at least two fractions using one or more knife edges pointing in a direction opposite to the trajectories of the material, said separation being carried out without any material previously rebounding from any wall; and (d) subdividing the incoming sifting gas current into at least two parts including a coarse fraction and a middle fraction and leading off said parts separately, the improvement comprising: (e) drawing off a partial current directly after the material charging point in a direction different from the influx direction of the sifting gas current, said partial current having a current momentum component in a direction opposite to the direction in which the material is propelled into the sifting gas current which has a value which is at least 1/10 of that of the momentum of the current of material being propelled into the sifting gas and carrying with said current a finest fraction; and (f) returning the portion of the sifting gas which is not drawn off as a partial current but which carries said middle fraction, after separation of said middle fraction, back to the incoming sifting gas.

Claim 25

In a method for sifting particulate material in a cross current comprising the steps of: (a) establishing a high velocity sifting gas current; (b) propelling the particles to be sifted into the sifting gas current at a separating zone with all the particles of the same size having the same velocity of at least approximately 5 m/sec at a material charging point in a thin layer transverse to the direction of the sifting gas current whereby said particles will spread out according to size based on their individual momentum and the current of the sifting gas; (c) after a time of flight of the order of magnitude of 1/100 sec. separating the spread out particles into at least two fractions using one or more knife edges pointing in a direction opposite to the trajectories of the material, said separation being carried out without any material previously rebounding from any wall; and (d) subdividing the incoming sifting gas current into at least two parts including a coarse fraction and a middle fraction and leading off said parts separately, the improvement comprising: (e) drawing off a partial current directly after the material charging point in a direction different from the influx direction of the sifting gas current, said partial current having a current momentum component in a direction opposite to the direction in which the material is propelled into the sifting gas current which has a value which is at least 1/10 of that of the momentum of the current of material being propelled into the sifting gas and carrying with said current a finest fraction; and (f) returning the portion of the sifting gas which is not drawn off as a partial current but which carries said middle fraction, after separation of said middle fraction, back to the incoming sifting gas.

Claim 26

In a method for sifting particulate material in a cross current comprising the steps of: (a) establishing a high velocity sifting gas current through a single influx duct to form a sifting gas current; (b) propelling the particles to be sifted into the sifting gas current at a separating zone with all the particles of the same size having the same velocity of at least approximately 5m/sec at a material charging point in a thin layer transverse to the direction of the sifting gas current whereby said particles will spread out according to size based on their individual momentum and the current of the sifting gas; (c) after a time of flight of the order of magnitude of 1/100 sec. separating the spread out particles into at least two fractions using one or more knife edges pointing in a direction opposite to the trajectories of the material, said separation being carried out without any material previously rebounding from any wall; (d) subdividing the incoming sifting gas current into at least two parts and leading off said parts separately, the improvement comprising: (e) drawing off a partial current directly after the material charging point in a direction different from the influx direction of the sifting gas current said partial current having a current momentum component in a direction opposite to the direction in which the material is propelled into the sifting gas current which the material is propelled into the sifting gas current which has a value which is at least 1/10 of that of the momentum of the current of material being propelled into the sifting gas; and (f) adjusting the velocity of the portion of the sifting gas which is drawn off as a partial current and the velocity of the sifting gas which is lead off separately in separate parts to be greater than the velocity of the sifting gas entering into the separating zone.

Claim 27

In a method for sifting particulate material in a cross current comprising the steps of: (a) establishing a high velocity sifting gas current through a single influx duct to form a sifting gas current; (b) propelling the particles to be sifted into the sifting gas current at a separating zone with all the particles of the same size having the same velocity of at least approximately 5m/sec at a material charging point in a thin layer transverse to the direction of the sifting gas current whereby said particles will spread out according to size based on their individual momentum and the current of the sifting gas; (c) after a time of flight of the order of magnitude of 1/100 sec. separating the spread out particles into at least two fractions using one or more knife edges pointing in a direction opposite to the trajectories of the material, said separation being carried out without any material previously rebounding from any wall; (d) subdividing the incoming sifting gas current into at least two parts and leading off said parts separately, the improvement comprising: (e) drawing off a partial current directly after the material charging point in a direction different from the influx direction of the sifting gas current said partial current having a current momentum component in a direction opposite to the direction in which the material is propelled into the sifting gas current which the material is propelled into the sifting gas current which has a value which is at least 1/10 of that of the momentum of the current of material being propelled into the sifting gas; and (f) adjusting the velocity of the portion of the sifting gas which is drawn off as a partial current and the velocity of the sifting gas which is lead off separately in separate parts to be greater than the velocity of the sifting gas entering into the separating zone.