This invention pertains generally to improved metal wood type golf club heads. A recent trend in golf club head design has been to increase the size of such heads to generate increased performance and create more “forgiving” golf clubs. Although this can be said to be true for golf clubs in general, it may be observed that wood type club heads in particular have increased in size dramatically over the past few years. This has presented a number of challenges in particular to designers of modern golf clubs of the “metal wood” variety, a detailed discussion of which is contained in the above referenced applications.
A metalwood head configuration that provides substantial advancements in performance, is proposed. The sound at impact of exemplary club heads in accordance with the teachings of the various embodiments of the present invention is deemed improved and more appealing in comparison to many performance wood-type clubs produced recently. In particular, a metallic ringing sound produced at impact, while different from that produced by conventional oversized metalwoods, is confidence inspiring to golfers and equates to an overall impression of quality and performance. The sound produced at impact by a golf club head is related to the structural response of the head. Hollow metal wood club heads having modified structural geometries that improve performance may exhibit structural responses that result in poor acoustical performance.
Therefore, structures are disclosed for improving the acoustical response of a hollow metalwood golf club heads having performance driven modifications to their head shape. These and other features, aspects, and advantages of the club head according to the invention in its various embodiments will become apparent after consideration of the ensuing description and the accompanying drawings.
Embodiments of the present invention will now be described, by way of example only, with reference to the following drawings in which:
For the purposes of illustration these figures are not necessarily drawn to scale. In all of the figures, like components may be designated by like reference numerals.
A club head 200 is shown in
Striking face portion 202 has a loft angle, which is the general angle striking face portion 202 forms relative to vertical when head 200 is resting in an address position. The extremities of crown 211 may be determined by viewing the club head from a top-down direction in a plane that is generally perpendicular to the loft angle, as illustrated in
Major crown portion 208 may be generally characterized as being displaced vertically lower than the adjacent portions of minor crown portion 210. Major crown portion 208 may be further characterized as having a surface contour that does not follow the surface contour of minor crown portion 210, whereby the bulk of major crown portion 208 is displaced vertically downward relative to adjacent portions of minor crown portion 210. In one embodiment of the invention, major crown portion 208 may be characterized further still as having a concave surface contour while minor crown portion may be characterized as having a generally convex curvature, whereby the bulk of major crown portion 208 is displaced vertically downward relative to adjacent portions of minor crown portion 210. Alternatively, the contour of portion 208 may be generally planar. Thus, head 200 may maintain similar to identical sole and striking face proportions to modern metal wood heads with a reduction in volume of about 15 to about 40 percent, depending on the surface contour selected for major crown portion 208. Further, an appreciable amount of club head 200's minimum structural mass is relocated vertically lower, resulting in an improved center of gravity position at a decreased structural mass, thereby allowing for the possibility of improved launch conditions even before discretionary mass is added to attain a desired finished mass of between about 190 g and about 215 g for a driver type metalwood. Additionally, by lowering major crown portion 208 there is a significant reduction of skirt 206's surface area, and hence a corresponding reduction in material required to form the skirt, and therefore a corresponding increase in head 200's weight budget. The increased weight budget may be strategically distributed to further improve head 200's mass properties, or to construct additional performance-enhancing structural features.
Implementation of a recessed crown configuration alone may affect the inherent structural properties of head 200. For example, head 200 may achieve the USGA mandated maximum coefficient of restitution (COR) of 0.830 using a similar face thickness, or thickness profile for a variable thickness face, as would be used in a conventionally shaped metalwood head of similar proportions, yet may exhibit reduced overall structural stiffness when manufactured using a similar process, e.g. thin-wall cast body and welded-in-place face insert. While maintaining equivalent ball speeds as those generated by a conventionally shaped head having the same COR, this reduction in stiffness may, for example, present challenges to club head designers with respect to the acoustical response of the head during use since the sound radiated from head 200 at impact may be directly related to structural response.
Modal analyses were performed on a variety of finite element models representing exemplary configurations of head 200, each within the parameters of the numerous variables presented in the applicant's aforementioned patent application. By way of example, it was found that with similar overall dimensions, proportions and wall thicknesses as those of a conventionally shaped metalwood club head, head 200 may exhibit a reduction of between about 25% to about 50% in the primary modal frequency. These reductions in primary modal frequencies may be significant since the primary modal frequency may, for example, be viewed as the fundamental frequency of the audible response generated by head 200 at impact with a golf ball, and may alter the perceived quality of the sound produced at impact.
Generally, the effect that a particular mode will have on the overall sound quality of head 200 depends in part on the radiation efficiency of the mode. Radiation efficiency may be affected by several factors, for example the geometry of the structural area the mode occupies, the size of the structural area occupied by the mode, and the amplitude of oscillation of the mode. For example, since it may be difficult to predict the effect geometry may have on sound radiation efficiency, it may be possible to reduce the radiation efficiency of a particular mode by limiting the surface area of the mode, reducing the amplitude of oscillation of the mode, increasing the frequency of the mode, or a combination of any or all of the above.
Further, the acoustic performance of head 200 may vary inversely with the volume of the head. For example, it was found that when head 200 was configured to approximate the proportions of a 420 cm3 driver type metalwood head, acoustic performance was deemed superior to that of a configuration which approximated the proportions of a 460 cm3 driver type head. This may be due to the additional reduction in structural stiffness as a result of the increased surface area of the individual portions of head 200 in combination with the inherently less rigid geometry of the recessed crown configuration.
In one embodiment, head 200 was configured to have a volume of 340 cm3, which corresponds to a conventional head displacing about 460 cm3. A finite element analysis was performed on the head to determine the modal response at impact with a golf ball. The first, second and third modes were found to have frequencies of about 1960 Hz, 2460 Hz and 2920 Hz, respectively. All three modes were situated on the major crown portion. The first sole mode was found to be at approximately 3800 Hz. An example of a conventional head displacing about 460 cm3 has first, second, and third modal frequency values of about 3940 Hz, 4010 Hz, and 4330 Hz, respectively, where the first and third modes are located on the crown and the second is located on the sole. Although head 200 exhibits improved launch conditions, and therefore greater carrying distance, in comparison to the exemplary conventional head, there is a significant reduction in the modal frequencies produced by impact. For many golfers, the sound of contemporary metalwood driver heads may be accepted and associated with good performance, therefore the difference in tones produced by head 200 may be unpleasant to some golfers and/or associated with poor performance, making acceptance of the club difficult.
Constraining member 402 may generally constrain at least a portion of head 300 whose structural properties result in radiation of unwanted sound energy that detracts from head 300's acoustic performance, when used to impact a golf ball. For example, constraining member 402 may constrain major crown portion 308 to skirt portion 306 (not shown). Alternatively, constraining member 402 may constrain major crown portion 308 to sole portion 304 alone (not shown). In another example, constraining member 402 may constrain major crown portion 402 to both sole portion 304 and skirt portion 306, as shown in
In another embodiment, cantilever member 404 extends along sole 304, as shown in
Further, hc may vary along the length of the cantilever member 404, generally decreasing in value towards end 406, as shown in
Generally, constraining member 402 may reduce the surface of major crown portion 308 that is effectively unconstrained, thereby reducing the area that may oscillate freely. Thus, constraining member 402 may decrease the area occupied by major crown portion 308's low frequency modes, and it may increase their frequencies, and may further reduce the amplitude of their oscillation. Cantilever member 404 may allow further tuning of the modal characteristics of major crown portion 308, for example by increasing the bending stiffness of the unconstrained area of the major crown portion, which may decrease the amplitude of oscillation and increase modal frequencies.
It may be particularly advantageous for cantilever member 404 to extend across the entire inner surface of major crown portion 308 as shown in
Constraining member 402 may be provided with at least one cut-out 410, an example of which is shown in
Typical hc values may range from between about 1 mm and about 10 mm. For heads having proportions similar to modern driver type club heads, e.g., about 300 to about 550 cm3, it may be advantageous to provide more than one structural modifying element.
In another example, for a head approximating the proportions of a typical fairway wood sized head, e.g. 100-190 cm3, it may be advantageous to use a single element 400, where height hc may range from about 2 mm to about 10 mm, and more preferably from about 3 mm to about 6 mm. A finite element simulation was performed on head 300 provided with two SRM elements 400 positioned as shown in
Although the benefits of implementing an SRM element comprising a constraining member and a cantilever member have been demonstrated for a head having a displaced crown configuration, it should be appreciated that the application of the element may not be limited solely to this head configuration. Similar needs for increased structural stiffness may be necessary for a variety of other head configurations. For example, as shown in
In some instances, sufficient reductions in radiation efficiency of low frequency modes may be obtained by providing metalwood heads with constraining members alone. Typically, in such instances a metalwood head 600, as shown in
Generally, an improved acoustic response may be achieved by limiting lsc to no more than 40% of ls and more preferably to between 10-40% of ls. In another aspect of the invention, it may be preferable to limit lsc to no more than 35% of ls. Furthermore, constraining member 610 may provide improvements to the acoustic response of head 600 when the ls value is greater than or equal to about 3.75 inches.
Further techniques which may be used to modify or enhance the structural response of a hollow metalwood head that has poor acoustic performance include localized thickening of a portion of the head in a region of high modal stress. The region of high modal stress to be thickened should be in the area occupied by the mode or modes which are affecting the acoustic performance of the head. Modal stress refers to the relative stress caused in a given portion of the head by modal oscillations. The greater the amplitude of oscillation, the higher the modal stress. Generally, the maximum stress induced by the low frequency modes may not be so high as to require thickening of the affected portion for structural reasons. In most cases, the actual stress values attributed to the displacement of the mode may be a small fraction of the failure strength of materials commonly used to produce hollow metalwood clubs, such as steel alloys, titanium alloys, composites, aluminum alloys, plastics, and the like. However, it was found that by thickening the head portion in the highest modal stress area of a particular mode, the modal frequency could be improved, or increased, about 100 to about 350 Hz in general, and in some cases even more. Additionally, the mode's amplitude was decreased and the overall radiation efficiency of the mode also reduced. Thus, thickening of high modal stress areas of portions containing low frequency modes which detract from the acoustic performance of any of the aforementioned heads may effectively be used to improve overall acoustic quality of said heads. Typical thickness increases that will prove effective may generally be about 20% to about 100% of the portion thickness, depending on the material being used and the modal stress values.
Similarly, when a low frequency mode which detracts from a given hollow metalwood head's acoustic performance is present proximate the junction of two or more portions of that head, a constraining member may be used to tie the portions together. This may be effective when the constraining member is allowed to pass through the region of highest modal stress, thereby effectively reducing the amplitude of oscillation of the mode, increasing the mode's frequency, and generally reducing the mode's radiation efficiency.
It should be appreciated that the structural response modifying elements disclosed herein may be formed integrally along with the various portions of a particular head, for example by casting, or may be manufactured separately and affixed within the head, for example by welding, adhesive bonding, mechanical fastening or any suitable joining technique. When manufactured separately from the head, it may be beneficial to use materials that provide weight and/or cost savings for their construction. As examples, plastics, fiber reinforced plastics, or low density metals such as aluminum and magnesium alloys may be used to form the elements.
The above-described embodiments of the club head are given only as examples. Therefore, the scope of the invention should be determined not by the illustrations given, but by the appended claims and their equivalents.
This application is a continuation of application Ser. No. 13/733,898, filed Dec. 31, 2012, which is a continuation of application Ser. No. 12/923,595, filed Sep. 29, 2010, which is a continuation of application Ser. No. 11/705,499, filed Feb. 13, now U.S. Pat. No. 7,854,666, which is a continuation-in-part of application Ser. No. 11/247,148 filed Oct. 12, 2005, now U.S. Pat. No. 7,651,414, which claims the benefits under 35 U.S.C. §119(e) of Provisional Application No. 60/617,659, filed Oct. 13, 2004 and Provisional Application No. 60/665,653, filed Mar. 25, 2005. This application also claims the benefits under 35 U.S.C. §119(e) of Provisional Application No. 60/772,881, filed Feb. 14, 2006. The entire contents of each of these prior applications are expressly incorporated herein by reference thereto.
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Entry |
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Golf Works (Maltby), The Golf Club Identification & Price Guide IV 1950-1998 (© 1999), p. 32-2. |
Photographs of internal structure of Nicklaus Air Bear 2 Clubhead (1997-1998). |
Number | Date | Country | |
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20150057102 A1 | Feb 2015 | US |
Number | Date | Country | |
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60772881 | Feb 2006 | US |
Number | Date | Country | |
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Parent | 13731898 | Dec 2012 | US |
Child | 14473499 | US | |
Parent | 12923595 | Sep 2010 | US |
Child | 13731898 | US | |
Parent | 11705499 | Feb 2007 | US |
Child | 12923595 | US |