The present invention relates to an improved golf club head. More particularly, the present invention relates to a golf club head with an improved striking face and improved shock absorption between the mating portions making up the body of the club head.
The complexities of golf club design are well known. The specifications for each component of the club (i.e., the club head, shaft, hosel, grip, and sub-components thereof) directly impact the performance of the club. Thus, by varying the design specifications, a golf club can be tailored to have specific performance characteristics.
The design of club heads has long been studied. Among the more prominent considerations in club head design are loft, lie, face angle, horizontal face bulge, vertical face roll, face progression, face size, sole curvature, center of gravity, material selection, and overall head weight. While this basic set of criteria is generally the focus of golf club engineering, several other design aspects must also be addressed. The interior design of the club head may be tailored to achieve particular characteristics, such as the inclusion of hosel or shaft attachment means, perimeter weights on the face or body of the club head, and fillers within hollow club heads.
Golf club heads must also be strong to withstand the repeated impacts that occur during collisions between the golf club and the golf ball. The loading that occurs during this transient event can accelerate the golf ball to several orders of magnitude greater than gravity. Thus, the club face and body should be designed to resist permanent deformation or catastrophic failure by material yield or fracture. Conventional hollow metal wood drivers made from titanium typically have a uniform face thickness exceeding 0.10 inch to ensure structural integrity of the club head.
Players generally seek a metal wood driver and golf ball combination that delivers maximum distance and landing accuracy. The distance a ball travels after impact may be dictated by variables including: the magnitude and direction of the ball's translational velocity; and, the ball's rotational velocity or spin. Environmental conditions, including atmospheric pressure, humidity, temperature, and wind speed, further influence the ball's flight. However, these environmental effects are beyond the control of the golf equipment manufacturer. Golf ball landing accuracy is driven by a number of factors as well. Some of these factors are attributed to club head design, such as center of gravity and club face flexibility.
The United States Golf Association (USGA), the governing body for the rules of golf in the United States, has specifications for the performance of golf balls. These performance specifications dictate the size and weight of a conforming golf ball. One USGA rule limits the golf ball's initial velocity after a prescribed impact to 250 feet per second ±2% (or 255 feet per second maximum initial velocity). To achieve greater golf ball travel distance, ball velocity after impact and the coefficient of restitution of the ball-club impact must be maximized while remaining within this rule.
Generally, golf ball travel distance is a function of the total kinetic energy imparted to the ball during impact with the club head, neglecting environmental effects. During impact, kinetic energy is transferred from the club and stored as elastic strain energy in the club head and as viscoelastic strain energy in the ball. After impact, the stored energy in the ball and in the club is transformed back into kinetic energy in the form of translational and rotational velocity of the ball, as well as the club. Since the collision is not perfectly elastic, a portion of energy is dissipated in club head vibration and in viscoelastic relaxation of the ball. Viscoelastic relaxation is a material property of the polymeric materials used in all manufactured golf balls.
Viscoelastic relaxation of the ball is a parasitic energy source, which is dependent upon the rate of deformation. To minimize this effect, the rate of deformation must be reduced. This may be accomplished by allowing more club face deformation during impact. Since metallic deformation may be purely elastic, the strain energy stored in the club face is returned to the ball after impact thereby increasing the ball's outbound velocity after impact.
A variety of techniques may be utilized to vary the allowable deformation of the club face, including uniform face thinning, thinned faces with ribbed stiffeners and varying thickness, among others. These designs should have sufficient structural integrity to withstand repeated impacts without permanent deformation of the club face. In general, conventional club heads also exhibit wide variations in the coefficient of restitution depending on the impact location on the face of the club. Furthermore, the accuracy of conventional clubs is highly dependent on impact location.
It has been reported in F. Werner and R. Greig, “How Golf Clubs Really Works and How to Optimize Their Designs”, Ch. 4, pp. 17-21 (2000) that a typical distribution of golf ball hits on the face of a driver club follows an elliptical pattern with its major axis orientating in a direction from high toe to low heel. The size of the hit distribution depends on the handicap of the golfer. Players with low handicap have smaller elliptical distribution and players with high handicap have larger elliptical distribution. These authors also patented golf clubs that have an elliptical outer hitting face that aligns in the direction of high toe to low heel. See U.S. Pat. No. 5,366,233, entitled “Golf Club Face for Drivers,” issued on Nov. 22, 1994. However, there is no teaching to align the coefficient of restitution of the golf club head to the ball impact pattern.
The present invention relates to a golf club head adapted for attachment to a shaft. The head includes a hitting face and a body. The hitting face is configured and dimensioned so that it includes at least an inner zone and a concentric intermediate zone. The inner zone has relatively high flexural stiffness and the intermediate zone has lower flexural stiffness. Preferably, the inner zone has a shape that comprises a major axis and a minor axis and the major axis aligns substantially in the direction of high heel to low toe. The inner zone can have an elliptical shape or a substantially parallelogram shape. The inner zone and intermediate zone may have same shape or different shape.
This arrangement of inner and intermediate zones forms an area of relatively high flexural stiffness in the direction of high heel to low toe, thereby creating high resilience in the direction of high toe to low heel. In other words, this arrangement creates a gradient of flexural stiffness in the direction of high toe to low heel, and produces a desirable effect of manipulating resilience or higher coefficient of restitution (COR) in that direction. This area of improved coefficient of restitution advantageously coincides with the ball impact pattern that golfers typically make on the hitting face.
The inventive club head encompasses a measurement zone that exhibits high COR where the lowest COR is at least 93% of the peak COR within this measurement zone. The measurement zone is defined by a rectangle having the dimensions of 0.5 inch by 1.0 inch, and the COR values are measured at the corners of the rectangle, the mid-points of the sides and the geometric center of the rectangle. The geometric center of the measurement zone preferably coincides with the geometric center of the face of the club.
The above is accomplished by providing the inner zone with a first flexural stiffness and the intermediate zone with a second flexural stiffness. Flexural stiffness is defined as Young's modulus or elastic modulus (E) times the zone's thickness (t) cubed or Et3. The first flexural stiffness is substantially higher than the second flexural stiffness. As a result, upon ball impact, the intermediate zone exhibits substantial elastic deformation to propel the ball.
In one embodiment, the first flexural stiffness is at least three times the second flexural stiffness. In other embodiments, the first flexural stiffness is six to twelve times the second flexural stiffness. More preferably, the first flexural stiffness is greater than 25,000 lb-in. Most preferably, the first flexural stiffness is greater than 55,000 lb-in. Preferably, the second flexural stiffness is less than 16,000 lb-in. More preferably, the second flexural stiffness is less than 10,000 lb-in.
Since the flexural stiffness is a function of material properties and thickness, the following techniques can be used to achieve the substantial difference between the first and second flexural stiffness: 1) different materials can be used for each portion, 2) different thicknesses can be used for each portion, or 3) different materials and thicknesses can be used for each portion.
The golf club head may further include a perimeter zone disposed between the intermediate zone and the body of the club. In one embodiment, the perimeter zone has a third flexural stiffness that is at least two times greater than the second flexural stiffness
In the club heads discussed above, the inner, intermediate and optional perimeter zones can have any shape that has a major axis and a minor axis, such as elliptical, rhombus, diamond, other quadrilateral shapes with one or more rounded corners and the like. The zones may also have a substantially parallelogram shape. Furthermore, the club head inner cavities can have a volume greater than about 100 cubic centimeters, and more preferably a volume greater than about 300 cubic centimeters. In other words, the club head in accordance to the present invention can be used in driver clubs and/or fairway clubs. In addition, the inner, intermediate, and perimeter zones can each have variable thickness.
Another feature of the present invention is locating the center of gravity of the club head with respect to a Cartesian coordinate system. The origin of the Cartesian coordinate system preferably coincides with the geometric center of the hitting face. The X-axis is a horizontal axis positioned tangent to the geometric center of the hitting face with the positive direction toward the heel of the club. The Y-axis is another horizontal axis orthogonal to the X-axis with the positive direction toward the rear of the club. The Z-axis is a vertical axis orthogonal to both the X-axis and Y-axis with the positive direction toward the crown of the club. The center of gravity is preferably located behind and lower than the geometric center of the face.
In one preferred embodiment, the center of gravity is spaced from the geometric center along the Z-axis by about −0.050 inch to about −0.150 inch, and more preferably by about −0.110 inch. The center of gravity is preferably spaced about ±0.050 inch, and more preferably about +0.015 inch from the geometric center along the X-axis. The center of gravity is preferably spaced about +2.0 inches and more preferably about +1.35 inches from the geometric center along the Y-axis.
The hitting face may comprise a face insert and a face support. The face support defines a cavity adapted to receive the face insert. The hitting face may further comprise at least one side wall, which can be a partial crown portion or a partial sole portion. Preferably, the inner zone is located on the face insert, and the intermediate zone may partially be located on the face insert and partially on the face support.
Another aspect of the invention provides for a crown portion to be composed of a material having a lower density than a body portion. The material for the crown portion selected from such materials as composite, thermoplastic or magnesium, and preferably graphite composite. The crown portion having an inner surface layer integrally composed of a vibration dampening or acoustical attenuating material. One embodiment would include a titanium mesh material.
An embodiment of the invention includes a non-integral dampening material, juxtaposed between the body and crown portions.
A preferred embodiment would be a gasket juxtaposed between the body and the crown portions
Yet still another embodiment of the invention is comprised of a body and light weight crown with a vibration dampening gap there between. The gap is preferably filled with putty or other shock absorption material such as a rubber based structural adhesive.
Preferred features of the present invention are disclosed in the accompanying drawings, wherein similar reference characters denote similar elements throughout the several views, and wherein:
a)-10(c) illustrate the results from a comparative example, which compares iso-COR contour lines of conventional golf club head and of an embodiment of the present invention;
a is a cross-section view of the crown portion attached to the lip section of the outer portion;
b is a plan view showing the layer of titanium mesh material integral with the inner surface of the crown portion;
c is a cross-section view of another embodiment of the crown portion wherein a titanium mesh ring is integral about the perimeter edge of the crown portion;
d is a plan view showing a ring of titanium mesh about the perimeter edge of the crown portion;
e is a cross-section view of an embodiment of the invention wherein a gasket is disposed between the lip section of the outer portion and the crown portion;
f is a plan view of the gasket of
g is a cross-section view of an embodiment of the invention having a gap filled with a shock absorption material between the crown portion and lip section;
h is a cross-section view of an embodiment of the invention having an “L” shaped gasket composed of a shock absorption material between the crown portion and lip section;
i is a cross-section view of an embodiment of the invention having a “Y” joint on the crown portion;
j is a plan view of the inner side of the crown portion showing the plurality of “Y” joints about the perimeter;
a is a front schematic depicting a 9 point spin variance across the front face of an embodiment of the invention; and
b is a front schematic depicting a 9 point spin variance across the front face of a prior art club head.
Referring to
A golf club shaft (not shown) is attached at hosel 24 and is disposed along a shaft axis SHA. The hosel may extend to the bottom of the club head or may terminate at a location between the top and bottom portions of the head. The hosel can also terminate flush with the top portion or extend into the cavity within the head.
Inner cavity 31 of club head 10 may be empty, or alternatively may be filled with foam or other low specific gravity material. It is preferred that the inner cavity 31 has a volume greater than 100 cubic centimeters, and more preferably greater than 300 cubic centimeters. In other words, the club head design in accordance to the present invention can be used with any driver club, as well as any fairway club. Preferably, the mass of the inventive club head is greater than 150 grams but less than 250 grams.
Referring to FIGS. 1 and 3-3D, the face 16 includes an inner zone or portion 36, an intermediate zone or surrounding portion 38 adjacent the inner zone 36, and an optional perimeter zone or outer portion 40. The intermediate zone 38 preferably surrounds inner zone 36, and the perimeter zone 40 preferably surrounds the intermediate zone 38. The inner zone 36 is a contiguous zone located on the hitting face 16 and contains a geometric center (“GC”) of the hitting face. As shown, inner zone 36 and its concentric zones have a generally elliptical shape with a major axis in the direction of high heel to low toe. As used herein, the term “ellipse” or “elliptical” refers to non-circular shapes that have discernable major axis and minor axis, and include, but are not limited to, any quadrilateral shapes, geometrical ellipses, quadrilateral shapes with one or more rounded corner(s) and unsymmetrical elliptical shapes. Also, the term “concentric” refers to shapes that substantially encircle or surround other shapes. The “major axis” is defined as the axis coinciding with the longest length that can be drawn through the non-circular shapes without intersecting the perimeter of the shapes at more than two locations, i.e., at the start and end points of said length. The “minor axis” is orthogonal to the major axis at or near its midpoint.
The major axis of inner portion 36 forms an angle, θ, with the shaft axis, SHA. Preferably, angle θ is between about 10° to about 60°, more preferably between about 20° and about 50°, and most preferably between about 25° and about 45°. Additionally, the ratio of the length of the major axis to the length of minor axis is preferably greater than 1.0 and more preferably less than about 6.0.
Preferably, zones 36, 38 and 40 are concentric to each other within hitting face 16. The inner zone 36 has a first thickness T1. The intermediate zone 38 has a second thickness T2. The first thickness T1 is greater than the second thickness T2. Typically, when the club head is cast, the perimeter zone 40 is thicker than the intermediate zone 38. Alternatively, the hitting face may also be forged. However, the present invention is not limited to any manufacturing technique. T1 may range from about 1.5 mm to about 7.5 mm and T2 may range from about 0.8 mm to about 3.0 mm. Preferably, the first thickness T1 is equal to about one and a half (1.5) times the thickness T2 to about four (4) times the thickness T2.
The thickness relationships between the zones 36, 38, and 40 are provided so that a predetermined relationship exists between flexural stiffness exhibited by each of the zones.
For clubs that have a hitting face made from a single material, such as titanium or titanium alloy, the area of highest thickness corresponds to the portion with the highest flexural stiffness. Flexural stiffness (FS) of each portion is defined as:
FS=E(t3),
where:
E is the elastic modulus or Young's modulus of the material of the portion, and t is the thickness of the portion.
Young's modulus of titanium is about 16.5×106 lbs/in2, and thickness is typically measured in inch. Hence, FS as used in this application has the unit of lb·in.
The inner zone 36 has a first flexural stiffness FS1. The intermediate zone 38 has a second flexural stiffness FS2. The perimeter zone 40 has a third flexural stiffness FS3. The predetermined relationship between the portions is that the first flexural stiffness FS1 is substantially greater than the second flexural stiffness FS2, and the optional third flexural stiffness FS3 is substantially greater than the second flexural stiffness FS2. Preferably, the first flexural stiffness FS1 is at least three times greater than the second flexural stiffness FS2, i.e., (FS1/FS2)≧3. When the above ratio of flexural stiffness is less than three, the inner zone sustains excessive deformation during impact and accuracy of the club is diminished. More preferably, the first flexural stiffness FS1 is about six (6) to twelve (12) times greater than the second flexural stiffness FS2. Most preferably, the first flexural stiffness FS1 is about eight (8) times greater than the second flexural stiffness FS2. Preferably, the third flexural stiffness FS3 is at least two times greater than the second flexural stiffness FS2, i.e., (FS3/FS2)≧2.
Alternatively, the flexural stiffness, FS1, FS2 or FS3, can be determined for two combined adjacent zones, so long as the preferred ratio (FS1/FS2)≧3 or (FS3/FS2)≧2 is satisfied. For example, FS1, can be calculated to include both zones 36 and 38, and FS3 can be calculated to include both zones 38 and 40.
The thickness of the zones, T1 and T2, may be constant within the zone as illustrated in
In club head 10 (as shown in
Quantitatively, it is preferred that the first flexural stiffness FS1 is greater than 25,000 lb-in. When the first flexural stiffness is less than 25,000 lb-in excessive deformation of the inner region can occur during impact and accuracy is diminished. More preferably, the first flexural stiffness FS1 is greater than 55,000 lb-in. Preferably, the second flexural stiffness FS2 is less than 16,000 lb-in. When the second flexural stiffness is greater than 16,000 lb-in, the resultant ball velocity is reduced. More preferably, the second flexural stiffness FS2 is less than 10,000 lb-in and, most preferably, less than 7,000 lb-in.
Referring to
Referring again to
The Cartesian coordinate system is defined as having the origin coincident with the geometric center of the hitting face. The hitting face is not a rectilinear plane, but due to the bulge and roll radii it is a curvilinear surface. The X-axis is a horizontal axis lying tangent to the geometric center of the hitting face with the positive direction toward the heel of the club. The Y-axis is another horizontal axis orthogonal to the X-axis with the positive direction toward the rear of the club. The Z-axis is a vertical axis orthogonal to both the X-axis and Y-axis with the positive direction toward the crown of the club.
The center of gravity is preferably located both behind and lower than the geometric center of the face, when the club head is resting on a flat surface (i.e., at its natural loft). In one preferred embodiment, the center of gravity of club head 10 is spaced from the geometric center along the Z-axis between about −0.050 inch and about −0.150 inch, more preferably about −0.110 inch. The center of gravity is preferably spaced about ±0.050 inch, more preferably about 0.015 inch, from the geometric center along the X-axis. The center of gravity is preferably spaced about 2.0 inches or less and more preferably about 1.35 inches or less from the geometric center along the Y-axis.
The center of gravity for the club head can be achieved by controlling the configuration and dimensions of the club head in addition to adding predetermined weights to the sole plate or to the club head. Other known methods of weight manipulation can be used to achieve the inventive center of gravity location as set forth above.
As shown in
In accordance to another aspect of the present invention, hitting face 16 may comprise a face insert 42 and face support 44, as shown in
In accordance to another aspect of the invention, the face insert may include one or more side walls, wherein the side walls may form part of the crown and/or part of the sole. As shown in
In this example, hitting face 16 has the following construction. The central zone 36 has a substantially parallelogram shape, as shown in
The test results were generated using computational techniques, which include finite element analysis models. In the computer model, the following assumptions were made: club head loft of 9°; club head mass of 195 grams; and club head material is 6AL-4V titanium alloy. The golf ball used in the model was a two-piece solid ball. Finite element models were used to predict ball launch conditions and a trajectory model was used to predict distance and landing area. The impact condition used for club coefficient of restitution (COR) tests was consistent with the USGA Rules for Golf, specifically, Rule 4-1e Appendix II Revision 2 dated Feb. 8, 1999.
Distributions of coefficient of restitution (COR) are shown in
COR or coefficient of restitution is one way of measuring ball resiliency. COR is the ratio of the velocity of separation to the velocity of approach. In this model, therefore, COR was determined using the following formula:
(vclub-post−vball-post)/(vball-pre−vclub-pre)
where,
COR, in general, depends on the shape and material properties of the colliding bodies. A perfectly elastic impact has a COR of one (1.0), indicating that no energy is lost, while a perfectly inelastic or perfectly plastic impact has a COR of zero (0.0), indicating that the colliding bodies did not separate after impact resulting in a maximum loss of energy. Consequently, high COR values are indicative of greater ball velocity and distance.
The iso-COR contour lines generated by the computational analysis are shown within a rectangle having dimensions of 0.5 inch by 1.0 inch, as typically used in the art. Within this rectangle, the inventive club head exhibits relatively high and substantially uniform COR values. The COR values are measured at nine points within this rectangle, i.e., the corners of the rectangle, mid-points of the sides and the geometric center of the rectangle. Additionally, the geometric center of this rectangular measurement zone preferably coincides with the geometric center of the hitting face of the club. In this example, the lowest COR within this measurement zone is 0.828 and the peak COR is 0.865. According to the present invention, the lowest COR is within 93% of the peak COR. This advantageously produces a hitting face with a substantially uniform COR and large “sweet spot.”
The iso-COR contour lines of the conventional club shown in
The iso-COR contour lines for the inventive club also follow an elliptical pattern, and as shown in
Without being limited to any particular theory, the inventors of the present invention observe that when an elliptical area of high thickness or high FS is present at or near the center of the hitting face with areas of less thickness or lower FS surrounding it, the iso-COR contour lines generally form an elliptical shape where the major axis of the iso-COR contours forms an angle with the major axis of the areas of high thickness or high FS. This arrangement of inner and intermediate zones forms a zone of relatively high flexural stiffness in the direction of high heel to low toe thereby creating high resilience in the direction of high toe to low heel. In other words, this arrangement creates a gradient of flexural stiffness in the direction of high toe to low heel and produces a desirable effect of manipulating resilience or higher coefficient of restitution (COR) in that direction. This area of improved coefficient of restitution advantageously coincides with the ball impact pattern that golfers typically make on the hitting face.
As shown is
The density range for crown portion 61 is from about 0.1 g/cc to 4.0 g/cc. Preferably the crown portion 61 may be formed from materials such as magnesium, graphite composite, a thermoplastic, but the preferred material for the crown portion 61 is graphite composite. Preferably, the crown portion 61 has a thickness in the range of about 0.1 mm to about 1.5 mm, and more preferably less than about 1.0 mm.
An embodiment of the invention is shown in
Another embodiment of the invention is described on
Another way to dampen vibrations according to the invention is shown in
The materials for forming the body portion 60 may be stainless steel, pure titanium or a titanium alloy. The more preferred material comprises titanium alloys, such as titanium 6-4 alloy, which comprises 6% aluminum and 4% vanadium. The body portion 60 may be manufactured through casting with a face insert, or formed portions with a face insert. The face insert is made by casting, machining sheet metal or forming sheet metal. Another embodiment can be created by forming a wrapped face, from forging, stamping, powdered metal forming, or metal-injection molding.
Tests were conducted on each of two golf clubs of the present invention. The only physical difference between the two clubs was that one of the clubs was manufactured with the shock absorption layer 66, as shown in
An embodiment of the invention provides an improvement in the percentage of club area relative to the head volume. With the composite crown portion 61 being considerably lighter than titanium, weight is removed from the crown and may then be redistributed into weight inserts in the body and face. The weight relocation helps to position the center of gravity lower. As seen in
As suggested above,
A significant performance criteria in the design of a golf club is the club's “forgiveness” or its ability to provide near optimum hitting for golf hits that are not struck right on the perfect “sweet spot” of the club. The “sweet spot” of a golf club is usually referred to as that spot on the club face wherein maximum Coefficient of Restitution is obtained. The golf club of the present invention provides a “sweet zone” or nine (9) points across the club face, in which the club will deliver near maximum COR, at not just one particular point on the club face, but at any point within the sweet zone.
a and 14b make a 9 point comparison of the club faces of a model 454 Cobra versus the ERC Fusion club of Callaway Golf Company. The spin of the golf ball coming off the club face is an important parameter and in a perfect situation, the spin would be the same for the entire club face. In the design of a club face, having a minimum variance of spin across a large area of the face is a highly desired performance characteristic. The performance data shown on
While various descriptions of the present invention are described above, it should be understood that the various features of each embodiment can be used alone or in any combination thereof. Therefore, this invention is not to be limited to only the specifically preferred embodiments depicted herein. Further, it should be understood that variations and modifications within the spirit and scope of the invention may occur to those skilled in the art to which the invention pertains. For example, the face and/or individual zones can have thickness variations in a step-wise or continuous fashion. Other modifications include a perimeter zone that has a thickness that is greater than or less than the adjacent, intermediate zone. In addition, the shapes of the central, intermediate, and perimeter zones are not limited to those disclosed herein. Accordingly, all expedient modifications readily attainable by one versed in the art from the disclosure set forth herein that are within the scope and spirit of the present invention are to be included as further embodiments of the present invention. The scope of the present invention is accordingly defined as set forth in the appended claims.
The present application is a continuation of U.S. patent application Ser. No. 12/243,374, filed on Oct. 1, 2008, now U.S. Pat. No. 7,553,242 which is a continuation of U.S. patent application Ser. No. 11/938,883, filed on Nov. 13, 2007 now U.S. Pat. No. 7,431,664, which is a continuation of U.S. patent application Ser. No. 11/510,791 filed Aug. 25, 2006, and now U.S. Pat. No. 7,297,072, which is a divisional of Ser. No. 10/799,118 filed Mar. 12, 2004, and now U.S. Pat. No. 7,214,142. The disclosures of the parent patent applications are incorporated herein in their entirety.
Number | Name | Date | Kind |
---|---|---|---|
1318325 | Klin | Oct 1919 | A |
1319233 | Mattern | Oct 1919 | A |
1437463 | Boye | Dec 1922 | A |
1467435 | Kinnear | Sep 1923 | A |
1525352 | Aitken | Feb 1925 | A |
1543691 | Beat | Jun 1925 | A |
1582836 | Link | Apr 1926 | A |
1589363 | Butchart | Jun 1926 | A |
1595589 | Tyler | Aug 1926 | A |
1605551 | Mattern | Nov 1926 | A |
1699874 | Buhrke | Jan 1929 | A |
1704119 | Buhrke | Mar 1929 | A |
1704165 | Buhrke | Mar 1929 | A |
1720867 | Webster et al. | Jul 1929 | A |
2034936 | Barnhart | Mar 1936 | A |
2087685 | Hackney | Jul 1937 | A |
3567228 | Lynn | Mar 1971 | A |
3571900 | Hardesty | Mar 1971 | A |
3625518 | Solheim | Dec 1971 | A |
3659855 | Hardesty | May 1972 | A |
3863932 | Lezatte | Feb 1975 | A |
3985363 | Jepson et al. | Oct 1976 | A |
4021047 | Mader | May 1977 | A |
4023802 | Jepson et al. | May 1977 | A |
4193601 | Reid, Jr. et al. | Mar 1980 | A |
4213613 | Nygren | Jul 1980 | A |
4214754 | Zebelean | Jul 1980 | A |
D267965 | Kobayashi | Feb 1983 | S |
4429879 | Schmidt | Feb 1984 | A |
4432549 | Zebelean | Feb 1984 | A |
4449707 | Hayashi et al. | May 1984 | A |
4451041 | Hayashi et al. | May 1984 | A |
4451042 | Hayashi et al. | May 1984 | A |
4465221 | Schmidt | Aug 1984 | A |
4471961 | Masghati et al. | Sep 1984 | A |
4489945 | Kobayashi | Dec 1984 | A |
4511145 | Schmidt | Apr 1985 | A |
4762324 | Anderson | Aug 1988 | A |
4792140 | Yamaguchi et al. | Dec 1988 | A |
4826172 | Antonious | May 1989 | A |
4842243 | Butler | Jun 1989 | A |
4913438 | Anderson | Apr 1990 | A |
4915385 | Anderson | Apr 1990 | A |
4915386 | Antonious | Apr 1990 | A |
4919430 | Antonious | Apr 1990 | A |
4919431 | Antonious | Apr 1990 | A |
4921252 | Antonious | May 1990 | A |
4928965 | Yamaguchi et al. | May 1990 | A |
4930781 | Allen | Jun 1990 | A |
4932658 | Antonious | Jun 1990 | A |
4955610 | Creighton et al. | Sep 1990 | A |
D312858 | Anderson et al. | Dec 1990 | S |
5000454 | Soda | Mar 1991 | A |
5024437 | Anderson | Jun 1991 | A |
5028049 | McKeighen | Jul 1991 | A |
5046733 | Antonious | Sep 1991 | A |
5056705 | Wakita et al. | Oct 1991 | A |
5060951 | Allen | Oct 1991 | A |
5067715 | Schmidt et al. | Nov 1991 | A |
5090702 | Viste | Feb 1992 | A |
5094383 | Anderson et al. | Mar 1992 | A |
5106094 | Desbiolles et al. | Apr 1992 | A |
5141230 | Antonious | Aug 1992 | A |
5163682 | Schmidt et al. | Nov 1992 | A |
5180166 | Schmidt et al. | Jan 1993 | A |
5183255 | Antonious | Feb 1993 | A |
5213328 | Long et al. | May 1993 | A |
5221087 | Fenton et al. | Jun 1993 | A |
5240252 | Schmidt et al. | Aug 1993 | A |
5242167 | Antonious | Sep 1993 | A |
5255918 | Anderson et al. | Oct 1993 | A |
5261663 | Anderson | Nov 1993 | A |
5261664 | Anderson | Nov 1993 | A |
5271621 | Lo | Dec 1993 | A |
5292129 | Long et al. | Mar 1994 | A |
5295689 | Lundberg | Mar 1994 | A |
5301945 | Schmidt et al. | Apr 1994 | A |
5303922 | Lo | Apr 1994 | A |
5318300 | Schmidt et al. | Jun 1994 | A |
5328184 | Antonious | Jul 1994 | A |
5344140 | Anderson | Sep 1994 | A |
5346218 | Wyte | Sep 1994 | A |
5351958 | Helmstetter | Oct 1994 | A |
5358249 | Mendralla | Oct 1994 | A |
5362047 | Shaw et al. | Nov 1994 | A |
5362055 | Rennie | Nov 1994 | A |
5366223 | Werner et al. | Nov 1994 | A |
5380010 | Werner et al. | Jan 1995 | A |
5390924 | Antonious | Feb 1995 | A |
5395113 | Antonious | Mar 1995 | A |
5397126 | Allen | Mar 1995 | A |
5401021 | Allen | Mar 1995 | A |
5405136 | Hardman | Apr 1995 | A |
5405137 | Vincent et al. | Apr 1995 | A |
5407202 | Igarashi | Apr 1995 | A |
RE34925 | McKeighen | May 1995 | E |
5417419 | Anderson et al. | May 1995 | A |
5417559 | Schmidt | May 1995 | A |
5423535 | Shaw et al. | Jun 1995 | A |
5429357 | Kobayashi | Jul 1995 | A |
5431396 | Shieh | Jul 1995 | A |
5433440 | Lin | Jul 1995 | A |
5447307 | Antonious | Sep 1995 | A |
5447309 | Vincent | Sep 1995 | A |
5451056 | Manning | Sep 1995 | A |
5460376 | Schmidt et al. | Oct 1995 | A |
5467983 | Chen | Nov 1995 | A |
5470069 | Schmidt et al. | Nov 1995 | A |
5474296 | Schmidt et al. | Dec 1995 | A |
5482279 | Antonious | Jan 1996 | A |
5497993 | Shan | Mar 1996 | A |
5505453 | Mack | Apr 1996 | A |
5509660 | Elmer | Apr 1996 | A |
5522593 | Kobayashi et al. | Jun 1996 | A |
5524331 | Pond | Jun 1996 | A |
5533729 | Leu | Jul 1996 | A |
5536006 | Shieh | Jul 1996 | A |
5547630 | Schmidt | Aug 1996 | A |
5549297 | Mahaffey | Aug 1996 | A |
5564994 | Chang | Oct 1996 | A |
5584770 | Jensen | Dec 1996 | A |
5595552 | Wright et al. | Jan 1997 | A |
5611741 | Schmidt et al. | Mar 1997 | A |
5611742 | Kobayashi | Mar 1997 | A |
D379393 | Kubica et al. | May 1997 | S |
5626530 | Schmidt et al. | May 1997 | A |
5643104 | Antonious | Jul 1997 | A |
5643108 | Cheng | Jul 1997 | A |
5643110 | Igarashi | Jul 1997 | A |
5649872 | Antonious | Jul 1997 | A |
5651409 | Sheehan | Jul 1997 | A |
5655976 | Rife | Aug 1997 | A |
5669827 | Nagamoto | Sep 1997 | A |
5669829 | Lin | Sep 1997 | A |
5674132 | Fisher | Oct 1997 | A |
D387113 | Burrows | Dec 1997 | S |
5695411 | Wright et al. | Dec 1997 | A |
5709614 | Horiba | Jan 1998 | A |
5709615 | Liang | Jan 1998 | A |
5711722 | Miyajima et al. | Jan 1998 | A |
5716292 | Huang | Feb 1998 | A |
5718641 | Lin | Feb 1998 | A |
5720673 | Anderson | Feb 1998 | A |
5743813 | Chen et al. | Apr 1998 | A |
5753170 | Muang | May 1998 | A |
5755624 | Helmstetter | May 1998 | A |
5755627 | Yamazaki et al. | May 1998 | A |
5762567 | Antonious | Jun 1998 | A |
5766092 | Mimeur et al. | Jun 1998 | A |
5766094 | Mahaffey et al. | Jun 1998 | A |
5766095 | Antonious | Jun 1998 | A |
5776011 | Su et al. | Jul 1998 | A |
5797807 | Moore | Aug 1998 | A |
5807190 | Krumme et al. | Sep 1998 | A |
5827132 | Bamber | Oct 1998 | A |
RE35955 | Lu | Nov 1998 | E |
D401652 | Burrows | Nov 1998 | S |
5830084 | Kosmatka | Nov 1998 | A |
5839975 | Lundberg | Nov 1998 | A |
5842934 | Ezaki et al. | Dec 1998 | A |
5851159 | Burrows | Dec 1998 | A |
5851160 | Rugge et al. | Dec 1998 | A |
5863261 | Eggiman | Jan 1999 | A |
5873791 | Allen | Feb 1999 | A |
5873795 | Wozny et al. | Feb 1999 | A |
D406294 | Burrows | Mar 1999 | S |
5888148 | Allen | Mar 1999 | A |
5890973 | Gamble | Apr 1999 | A |
D411272 | Burrows | Jun 1999 | S |
5908357 | Hsieh | Jun 1999 | A |
5921872 | Kobayashi | Jul 1999 | A |
5931746 | Soong | Aug 1999 | A |
5935019 | Yamamoto | Aug 1999 | A |
5938541 | Allen et al. | Aug 1999 | A |
5941782 | Cook | Aug 1999 | A |
5944619 | Cameron | Aug 1999 | A |
5954596 | Noble et al. | Sep 1999 | A |
D415807 | Werner et al. | Oct 1999 | S |
5961394 | Minabe | Oct 1999 | A |
5967905 | Nakahara et al. | Oct 1999 | A |
5971868 | Kosmatka | Oct 1999 | A |
5993329 | Shich | Nov 1999 | A |
6007432 | Kosmatka | Dec 1999 | A |
6027416 | Schmidt et al. | Feb 2000 | A |
6139445 | Werner et al. | Oct 2000 | A |
6143169 | Lee | Nov 2000 | A |
6152833 | Werner et al. | Nov 2000 | A |
6248025 | Murphy | Jun 2001 | B1 |
6319150 | Werner et al. | Nov 2001 | B1 |
6338683 | Kosmatka | Jan 2002 | B1 |
6354962 | Galloway et al. | Mar 2002 | B1 |
6368234 | Galloway | Apr 2002 | B1 |
6381828 | Boyce | May 2002 | B1 |
6390933 | Galloway | May 2002 | B1 |
6398666 | Evans et al. | Jun 2002 | B1 |
6435982 | Galloway et al. | Aug 2002 | B1 |
6506129 | Chen | Jan 2003 | B2 |
6605007 | Bissonnette et al. | Aug 2003 | B1 |
6626769 | Lin | Sep 2003 | B1 |
6648774 | Lee | Nov 2003 | B1 |
6663501 | Chen | Dec 2003 | B2 |
6669576 | Rice | Dec 2003 | B1 |
6755627 | Chang | Jun 2004 | B2 |
6776726 | Sano | Aug 2004 | B2 |
6994636 | Hocknell et al. | Feb 2006 | B2 |
7029403 | Rice et al. | Apr 2006 | B2 |
7137906 | Tsunoda et al. | Nov 2006 | B2 |
7211006 | Chang | May 2007 | B2 |
7214142 | Meyer et al. | May 2007 | B2 |
7297072 | Meyer et al. | Nov 2007 | B2 |
7431664 | Meyer et al. | Oct 2008 | B2 |
7553242 | Meyer et al. | Jun 2009 | B2 |
20020160854 | Beach et al. | Oct 2002 | A1 |
20040048681 | Nishio | Mar 2004 | A1 |
20040157678 | Kohno | Aug 2004 | A1 |
20040266548 | Cheng et al. | Dec 2004 | A1 |
Number | Date | Country |
---|---|---|
1114911 | Jan 1996 | CN |
2268693 | Jan 1994 | GB |
2331938 | Jun 1999 | GB |
59207169 | Nov 1984 | JP |
61033682 | Feb 1986 | JP |
61162967 | Jul 1986 | JP |
61181477 | Aug 1986 | JP |
61185281 | Aug 1986 | JP |
61240977 | Oct 1986 | JP |
1244770 | Sep 1989 | JP |
02130519 | May 1990 | JP |
4020357 | Jan 1992 | JP |
4327864 | Nov 1992 | JP |
5212526 | Aug 1993 | JP |
05237207 | Sep 1993 | JP |
6007487 | Jan 1994 | JP |
06031016 | Feb 1994 | JP |
6114126 | Apr 1994 | JP |
6126002 | May 1994 | JP |
6154367 | Jun 1994 | JP |
6182005 | Jul 1994 | JP |
6269518 | Sep 1994 | JP |
8168541 | Jul 1996 | JP |
8243194 | Sep 1996 | JP |
8280853 | Oct 1996 | JP |
8280854 | Oct 1996 | JP |
8294550 | Nov 1996 | JP |
9028842 | Feb 1997 | JP |
9047531 | Feb 1997 | JP |
9154985 | Jun 1997 | JP |
9168613 | Jun 1997 | JP |
9192270 | Jul 1997 | JP |
9192273 | Jul 1997 | JP |
9239074 | Sep 1997 | JP |
9239075 | Sep 1997 | JP |
9248353 | Sep 1997 | JP |
2717759 | Nov 1997 | JP |
9294833 | Nov 1997 | JP |
9299519 | Nov 1997 | JP |
10024126 | Jan 1998 | JP |
10024128 | Jan 1998 | JP |
10085369 | Apr 1998 | JP |
10118227 | May 1998 | JP |
10137372 | May 1998 | JP |
10155943 | Jun 1998 | JP |
10258142 | Sep 1998 | JP |
10263121 | Oct 1998 | JP |
10323410 | Dec 1998 | JP |
10337347 | Dec 1998 | JP |
Number | Date | Country | |
---|---|---|---|
20090227392 A1 | Sep 2009 | US |
Number | Date | Country | |
---|---|---|---|
Parent | 10799118 | Mar 2004 | US |
Child | 11510791 | US |
Number | Date | Country | |
---|---|---|---|
Parent | 12243374 | Oct 2008 | US |
Child | 12469058 | US | |
Parent | 11938883 | Nov 2007 | US |
Child | 12243374 | US | |
Parent | 11510791 | Aug 2006 | US |
Child | 11938883 | US |