STEEL CORD WITH ADAPTED ELONGATION PROPERTIES
20240352670 ยท 2024-10-24
Assignee
Inventors
Cpc classification
D07B3/00
TEXTILES; PAPER
D07B2205/305
TEXTILES; PAPER
D07B2801/10
TEXTILES; PAPER
D07B2801/10
TEXTILES; PAPER
D07B1/0613
TEXTILES; PAPER
D07B2207/208
TEXTILES; PAPER
D07B2207/4072
TEXTILES; PAPER
D07B2201/1044
TEXTILES; PAPER
D07B2201/2006
TEXTILES; PAPER
D07B2205/305
TEXTILES; PAPER
International classification
Abstract
In a tire the strength of steel cord and the resilience of rubber are a successful combination. However, in some specific areas of a tire, more elongation is expected from the steel cord, while still a sufficient degree of stiffness is expected. A steel cord is presented that has these properties. The steel cord comprises two or more steel elements that are twisted together. The steel elements comprise one or more steel filaments. In total the steel cord comprises N filaments, each with a cross sectional area A. When the steel elements are individualised out of the steel cord they show a helix pitch length of L.sub.o, while a single pitch has a centre line length of S. The inventive steel cord shows a P value of at least 50 newton, wherein P=NE (A/S).sup.2. Further methods are presented to produce this steel cord.
Claims
1-19. (canceled)
20. A steel cord for the reinforcement of a rubber product comprising two or more steel elements twisted together, said steel elements comprising one or more steel filaments, said steel cord comprising in total N steel filaments, each of said steel filaments having a cross sectional area A expressed in square millimeters said steel elements have, after individualization and under a tension of half a newton per filament in said steel element, a center line, said center line having a helix shape with a helix pitch length L.sub.o in millimeter, wherein the length of the center line of the steel element over one pitch is S millimeter, wherein the quantity P expressed newton:
21. The steel cord according to claim 20, said filaments have an equivalent diameter d defined by A=d.sup.2/4, wherein S/d is smaller than 30.
22. The steel cord according to claim 20, wherein the ratio L.sub.o/S is smaller than 0.95.
23. The steel cord according to claim 20, wherein the filaments of said steel cord, when in closed condition, have a pitch length of L.sub.o in millimeter, wherein the ratio L.sub.o/S is larger than 0.98.
24. The steel cord according to claim 23, wherein the structural elongation .sub.0 defined as (L.sub.oL.sub.0)/L.sub.o is larger than 3.5 per cent and smaller than 10 per cent.
25. The steel cord according to claim 20, wherein the force at the structural elongation .sub.0 is larger than 50 N and smaller than 120 N.
26. The steel cord according to claim 20, wherein the number of steel elements is two, three or four and wherein the number of steel filaments within one steel element is one, two or three.
27. The steel cord according to claim 20, wherein the number of filaments N is from and including 2 to 8 included.
28. A method to produce a steel cord comprising the following steps: (a) unwinding a number of steel elements with diameter de from spools; (b) providing a mandrel wire of diameter D; (c) twisting said steel elements around said mandrel wire with a cord number of twists N.sub.e per unit length in a cord twist direction thereby forming an intermediate cord; (d) removing the mandrel wire from said intermediate cord by turning said mandrel cord out of said intermediate cord, resulting in the steel cord; (e) winding the steel cord on a take-up spool.
29. The method according to claim 28, wherein the intermediate cord is wound on an intermediate spool after step (c) and unwound from said intermediate spool for performing step (d).
30. The method according to claim 28, wherein the intermediate cord is directly led from step (c) to step (d).
31. The method according to claim 28, wherein the step of removing the mandrel wire from said intermediate cord by turning said mandrel wire out of said intermediate cord is performed by moving said intermediate cord linearly; turning said mandrel wire out of said intermediate cord through a flyer relatively rotating around said intermediate cord thereby leaving the steel elements as a steel cord; winding the mandrel wire on a driven mandrel spool; winding said steel cord on a driven take-up spool.
32. The method of claim 31, wherein said driven take-up spool is inside said flyer or wherein said driven mandrel spool is inside said flyer.
33. The method according to claim 28, wherein the steel elements are steel filaments and the ratio of D/d.sub.e is larger than or equal to 0.8 and smaller than or equal to 2.
34. The method according to claim 28, wherein the steel element is a plurality of steel filaments and the ratio of D/d.sub.e is larger than or equal to 0.5 and smaller than or equal to 1.2.
35. The method according to claim 28, wherein the steel filaments in said steel elements of said intermediate cord are twisted to a steel element twist number N.sub.e in the cord twist direction, said element twist number being larger or equal than said cord twist number Ne and wherein said cord twist number Ne is larger than 150 twists per meter.
36. The method according to claim 28, wherein the filaments in said elements of said steel cord are twisted to an element twist number N.sub.e in the cord direction, said element twist number being smaller than said cord twist number.
37. The method according to claim 28, wherein said mandrel wire is one out of the group comprising: a metal wire, a steel wire, a steel cord, an organic yarn, an organic cord, an organic filament.
38. The method according to claim 28, wherein the combination of the total number N of steel filaments, wherein each of said steel filaments has a cross sectional area A expressed in square millimeters said steel elements having, after individualisation and under tension of half a newton per filament in said steel element, a center line, said center line having a helix shape, wherein the length of the center line of the steel element over one pitch is S in millimeter, is such that the quantity P expressed in newton:
Description
BRIEF DESCRIPTION OF FIGURES IN THE DRAWINGS
[0062]
[0063]
[0064]
[0065]
[0066]
[0067] Figures are provided with reference signs of which the unit and tens digit refers to similar items across figures and the hundred digit refers to the number of the figure.
MODE(S) FOR CARRYING OUT THE INVENTION
[0068] A first method of manufacturing is presented in
[0069] In order to remove the residual torsions from the steel elements twisted around the mandrel wire, the assembly is fed through a false twister 324 for plastically overtwisting the steel elements. The resulting intermediate cord 304 is free or practically free of residual torsions and is wound on an intermediate spool 302.
[0070] The steel elements comprise two, or three steel filaments that are twisted together with a lay length in a lay direction resulting in n.sub.e twists per meter. A typical value is from 25 to 150 twists per meter for the steel elements. The mandrel wire acts as a moving deformation pin, thorn, mandrel . . . around which the steel elements are plastically formed. It allows to give much higher degrees of plastic deformation of the steel elements than would be possible with conventional preforming systems. Moreover, by the use of a mandrel wire it becomes possible to deform also steel elements that are in the form of a strands. Strands cannot be deformed with e.g. preforming pins.
[0071] The final number of plastic twists N.sub.e that after the bunching steps are present in the steel elements is thus n.sub.e+N.sub.c. Typically this number will be smaller than 300 twists per meter. It will be nearing zero if n.sub.e=N.sub.c that is the steel elements is made with the same number of twists as that cord number twists but are twisted in the opposite direction.
[0072] In a further step of the method, as illustrated in
[0073] In an alternative embodiment of the method depicted in
[0074] Turning now to the product properties,
[0075] The sectional area of the steel filament can be easily established by measuring the diameter of the steel filaments and calculating the surface. The number of filaments N can be found by counting them.
[0076] The length of the centreline S can be determined by an axial scanning apparatus as described in WO 95/16816 or similar apparatus IM6000 obtainable from KEYENCE. The apparatus comprises two axially aligned chucks, 100 to 500 mm apart, for holding the individualised steel element at its ends during the test. A controlled tension is applied to the steel element of half a newton per filament in the steel element by means of weight. A linear scanning apparatus such as a KEYENCE LS 3034 laser scan system in combination with a KEYENCE LS 3100 processing unit is made to travel parallel to the axis of the steel element by means of an encoding high precision linear drive (accuracy is better than 10 m at a step size of 50 m). The measurement plane of the laser scan system is perpendicular to the Z-axis. The laser scan system can scan the outer edges of the steel element up to a precision of 0.5 m.
[0077] In a first scan at the equidistant discrete measuring positions z.sub.j, z apart, the lower and upper edges of the steel element are determined and the average of both is used as the position of the centreline along the axis perpendicular to the Z-axis, i.e. the X-axis. In this way the positions x(z.sub.j) are measured and stored in a computer. The index j is the sequential number of the sampled.
[0078] Then the chucks are turned 90 and the scan is repeated. Now, the values y(z.sub.j) along the Y-axis, perpendicular to X and Z-axis are measured and stored. In this way the triplets (x(z.sub.j), y(z.sub.j), z.sub.j) are obtained that determine the shape of the centreline of the steel element. As this shape is substantially a helix the curves (z.sub.j, x(z.sub.j)) and (z.sub.j, y(z.sub.j)) are similar to a cosine and sine as a function of z.sub.j. The start of the first turn and the end of the last turn can be determined and this is the axial length l over which n helix pitches are counted. This axial length covers m measuring points
[0079] Now the total length s of the centreline over the axial length l can be calculated by adding the m1 measured sections:
[0080] The length of the center line of the steel element over one pitch S is thus equal to s/n. In the same manner the helix pitch length L.sub.o is equal to l/n. As the number n of helix turns measured is readily larger than 50 or even 100, the numbers S and L.sub.o are averages over a large number of helix turns.
[0081] The relation between the geometrical parameters L.sub.o, L.sub.c, S and the load-elongation diagram is illustrated in
[0082] When a tangent line (shown dashed) is drawn to the straight part of the curve, this can be extended towards the elongation axis 206. The crossing corresponds to the structural elongation .sub.0 as at this point the steel elements are closed and reach the corresponding helix pitch L.sub.c. That this point indeed corresponds to the closing of the steel elements can be demonstrated by imagining that the steel elements have an increasing modulus: all the corresponding tangent curves will go through the point (0, .sub.0) as the slope of the tangent line rises to vertical. When the steel cord is further stretched over 60, the ratio (L/S) remains constant while both L and S further increase due the elongation of the steel.
[0083] For the purpose of this application, the ratio (L.sub.c/S) is calculated as:
wherein d is the equivalent diameter of the steel filament.
[0084] When now considering an individualized steel element, a curve akin to 204 is obtained. But here the crossing with the L axis corresponds to a fully stretched helix that is a helix with length S. The elongation is then (SL.sub.o)/L.sub.0.
[0085] In a series of experiments, samples were prepared according the method depicted in
[0091] Note: the lay direction of filaments in the steel element and the lay direction of the steel element in the steel cord where identical and in the S direction.
[0092] The different geometrical and mechanical properties following have all been obtained on the final steel cord, that is the steel cord wherefrom the mandrel wire has been removed: [0093] (a) N is simply the number of steel filaments in the steel cord; [0094] (b) A1000 is the cross sectional area of a single steel filament expressed in mm.sup.2 times 1000. [0095] (c) S is the length of the centre line in one helix pitch according the described measurement procedure; [0096] (d) L.sub.o is the axial length of one helix pitch according the described measurement procedure; [0097] (e) P is the quantity calculated according the definition of the claim; [0098] (f) S/d is the ratio of S divided by the equivalent diameter of the steel filament; [0099] (g) L.sub.o/S and L.sub.c/S are the ratios of the indicated quantities; [0100] (h) .sub.0 is the structural elongation as determined by the procedure of
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TABLE-US-00001 TABLE I N.sub.e N.sub.c A 1000 S L.sub.o P .sub.o F (.sub.o) Ref. Construction (t/m) (t/m) D/d.sub.e N (in mm.sup.2) (in mm) (in mm) (in N) S/d L.sub.o/S L.sub.c/S (in %) (in N) 522 0.4 + 2 (2 0.225) 300 200 0.89 4 39.761 5.731 5.382 121 25.5 0.939 0.985 5.79 78.86 507 0.4 + 4 (2 0.225) 300 200 0.89 8 39.761 5.790 5.259 237 25.7 0.908 0.948 4.77 101.67 523 0.4 + 2 0.225 200 200 1.78 2 39.761 5.961 5.589 56 26.5 0.938 0.993 5.19 52.47 503 0.4 + 4 0.225 200 200 1.78 4 39.761 5.977 5.669 111 26.6 0.949 0.986 3.96 74.04 521 0.3 + 4 0.225 200 200 1.33 4 39.761 5.528 5.302 130 24.6 0.959 0.984 2.00 52.29 524 0.3 + 2 0.15 200 200 2.00 2 17.671 5.926 5.793 11 39.5 0.978 0.997 1.14 12.02 514 0.35 + 3 0.15 133 133 2.33 3 17.671 9.284 9.202 7 61.9 0.991 0.998 0.37 7.21 509 0.35 + 3 (2 0.15) 200 133 1.17 6 17.671 8.940 8.812 15 59.6 0.986 0.994 0.77 17.03