WO2010137345A1 - 共鳴器の設計方法及び共鳴器を具える空気入りタイヤ - Google Patents
共鳴器の設計方法及び共鳴器を具える空気入りタイヤ Download PDFInfo
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- WO2010137345A1 WO2010137345A1 PCT/JP2010/003615 JP2010003615W WO2010137345A1 WO 2010137345 A1 WO2010137345 A1 WO 2010137345A1 JP 2010003615 W JP2010003615 W JP 2010003615W WO 2010137345 A1 WO2010137345 A1 WO 2010137345A1
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- Prior art keywords
- resonator
- circumferential groove
- groove
- branch
- branch groove
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Classifications
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- B—PERFORMING OPERATIONS; TRANSPORTING
- B60—VEHICLES IN GENERAL
- B60C—VEHICLE TYRES; TYRE INFLATION; TYRE CHANGING; CONNECTING VALVES TO INFLATABLE ELASTIC BODIES IN GENERAL; DEVICES OR ARRANGEMENTS RELATED TO TYRES
- B60C11/00—Tyre tread bands; Tread patterns; Anti-skid inserts
- B60C11/03—Tread patterns
-
- B—PERFORMING OPERATIONS; TRANSPORTING
- B60—VEHICLES IN GENERAL
- B60C—VEHICLE TYRES; TYRE INFLATION; TYRE CHANGING; CONNECTING VALVES TO INFLATABLE ELASTIC BODIES IN GENERAL; DEVICES OR ARRANGEMENTS RELATED TO TYRES
- B60C19/00—Tyre parts or constructions not otherwise provided for
- B60C19/002—Noise damping elements provided in the tyre structure or attached thereto, e.g. in the tyre interior
-
- B—PERFORMING OPERATIONS; TRANSPORTING
- B60—VEHICLES IN GENERAL
- B60C—VEHICLE TYRES; TYRE INFLATION; TYRE CHANGING; CONNECTING VALVES TO INFLATABLE ELASTIC BODIES IN GENERAL; DEVICES OR ARRANGEMENTS RELATED TO TYRES
- B60C11/00—Tyre tread bands; Tread patterns; Anti-skid inserts
- B60C11/03—Tread patterns
- B60C11/0306—Patterns comprising block rows or discontinuous ribs
-
- B—PERFORMING OPERATIONS; TRANSPORTING
- B60—VEHICLES IN GENERAL
- B60C—VEHICLE TYRES; TYRE INFLATION; TYRE CHANGING; CONNECTING VALVES TO INFLATABLE ELASTIC BODIES IN GENERAL; DEVICES OR ARRANGEMENTS RELATED TO TYRES
- B60C11/00—Tyre tread bands; Tread patterns; Anti-skid inserts
- B60C11/03—Tread patterns
- B60C11/04—Tread patterns in which the raised area of the pattern consists only of continuous circumferential ribs, e.g. zig-zag
-
- B—PERFORMING OPERATIONS; TRANSPORTING
- B60—VEHICLES IN GENERAL
- B60C—VEHICLE TYRES; TYRE INFLATION; TYRE CHANGING; CONNECTING VALVES TO INFLATABLE ELASTIC BODIES IN GENERAL; DEVICES OR ARRANGEMENTS RELATED TO TYRES
- B60C11/00—Tyre tread bands; Tread patterns; Anti-skid inserts
- B60C11/03—Tread patterns
- B60C2011/0337—Tread patterns characterised by particular design features of the pattern
- B60C2011/0339—Grooves
- B60C2011/0341—Circumferential grooves
-
- B—PERFORMING OPERATIONS; TRANSPORTING
- B60—VEHICLES IN GENERAL
- B60C—VEHICLE TYRES; TYRE INFLATION; TYRE CHANGING; CONNECTING VALVES TO INFLATABLE ELASTIC BODIES IN GENERAL; DEVICES OR ARRANGEMENTS RELATED TO TYRES
- B60C11/00—Tyre tread bands; Tread patterns; Anti-skid inserts
- B60C11/03—Tread patterns
- B60C2011/0337—Tread patterns characterised by particular design features of the pattern
- B60C2011/0339—Grooves
- B60C2011/0381—Blind or isolated grooves
-
- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y10—TECHNICAL SUBJECTS COVERED BY FORMER USPC
- Y10T—TECHNICAL SUBJECTS COVERED BY FORMER US CLASSIFICATION
- Y10T29/00—Metal working
- Y10T29/49—Method of mechanical manufacture
Definitions
- the present invention relates to a pneumatic tire, which reduces noise generated from the pneumatic tire, improves quietness, and improves braking performance, drainage performance and driving stability on a wet road surface.
- the tire noise around 1000 Hz is mainly generated by air column resonance.
- the air column resonance sound is noise generated by resonance of air in a pipe surrounded by a circumferential groove continuously extending in the circumferential direction of the tread surface and a road surface, and is 800 to 1200 Hz in a general passenger car. It is often observed to a certain extent, and since the peak sound pressure level is high and the frequency band is wide, it accounts for most of the noise generated from pneumatic tires.
- FIG. 1 there is a circumferential groove in the grounding surface, and when the length of the circumferential groove in the grounding surface is L under normal internal pressure / load load conditions, the air generated from the circumferential groove.
- the resonance frequency (Hz) of the medium resonance sound is It can ask for.
- n corresponds to the nth-order resonance
- c represents the speed of sound in the air.
- n 1
- Patent Document 1 A long horizontal groove (side-branch type resonator) with one end opened in the circumferential groove and the other end terminated in the land, and anti-resonance in the resonator is used to reduce air column resonance. It has been proposed to let However, there is a demand for improved drainage performance of pneumatic tires having a reduced groove volume in the circumferential groove. Further, in the pneumatic tire described in Patent Document 1, since it is essential to dispose a long lateral groove, the degree of freedom in designing the tread pattern is improved, and the rigidity of the land portion is ensured to ensure the handling stability.
- a branch groove part branched from the tire circumferential groove and a cross-sectional area connected to the branch groove part and orthogonal to the extending direction are larger than the branch groove part.
- a technique has also been proposed in which a Helmholtz type resonator having an air chamber is disposed to reduce air column resonance using antiresonance by the resonator (see FIG. 4).
- the frequency of Helmholtz type resonators is It is expressed by Here, S is the cross-sectional area of the thin tube, l h is the length of the thin tube, and V is the volume of the air chamber.
- S is the cross-sectional area of the thin tube
- l h is the length of the thin tube
- V is the volume of the air chamber.
- the frequency of a simple resonator can be estimated by Formula 4 and 5, in general shape, it is disclosed by patent document 3 and can consider with the step type resonator as shown in FIG. desirable.
- l 1 and l 2 represent the length of the tube
- S min and S max represent the cross-sectional area of the tube, respectively.
- Equation 6 can be used in general design, the analytical solution cannot be obtained from here because the formula is transcendental. Accordingly, trial and error are required several times at the design stage of the resonator, time and effort are required for the design, and the efficiency is poor. In addition, it has been unclear how stable the resonator acts against fluctuations in the contact length of the circumferential groove until the tire including the resonator is run and tested. For generally complicated shapes, as disclosed in Patent Documents 4 and 5, it is possible to obtain the resonance frequency of the resonator using numerical calculation. However, due to problems such as man-hours for creating a calculation model, a simpler resonator design method is desired.
- an object of the present invention is to provide a method for designing a resonator more easily by deriving a model formula that does not transcend the formula.
- a further object of the present invention is to provide a pneumatic tire including a resonator designed by such a design method.
- a method for designing a resonator according to the present invention includes: a tread portion tread having at least one circumferential groove extending in a tire circumferential direction; and a pipe in a pipe formed by the circumferential groove and a road surface.
- the resonator has a resonator for reducing noise generated by resonance, and the resonator has a branch groove part extending from the circumferential groove and an area of a cross section connected to the branch groove part and perpendicular to the extending direction.
- the length of the central axis O-O 'of the branch groove is set to l in the ground road surface of the circumferential groove.
- the position l 1 is circumferentially branch groove is S min of the cross-sectional area of the air chamber a from the opening of the groove l 1 / L ⁇ 1 / ⁇ , and, l 2 / L ⁇ (l -l 1) L ⁇ a 1 / [pi, and the shape l / L of the resonator, the relationship of S min / S max, When, It is characterized by designing the resonator so that
- the term “circumferential groove” as used herein refers to not only a groove extending linearly in the tire circumferential direction, but also a groove extending in a zigzag shape or a wave shape and making a round in the tire circumferential direction as a whole tire.
- the above l (l 1 , l 2 ), L, S min , S max are standard air pressures (atmospheric pressure: 1 atm) defined by JATMA, ETRTO, TRA, etc. at room temperature (generally 20 ° C.). Under normal conditions, the pneumatic tire is subjected to a load.
- the pneumatic tire of the present invention includes at least one circumferential groove extending in the tire circumferential direction on the tread portion tread surface, and reduces noise generated by resonance in the pipe formed by the circumferential groove and the road surface.
- the resonator has a branch groove extending from the circumferential groove, and the cross-sectional area connected to the branch groove and perpendicular to the extending direction is larger than that of the branch groove.
- the position l 1 where the branch groove portion becomes S min is l 1 / L ⁇ from the opening to the circumferential groove. 1 / a [pi, and, l 2 / L ⁇ (l -l 1) was / L ⁇ 1 / [pi, and the resonator geometry l And L, the relationship between the S min / S max, When, It is characterized by satisfying.
- (A) is a development view of a part of a tread portion including a side branch type resonator
- (b) is a cross-sectional view taken along line A-A ′ of the development view shown in (a). It is a figure which shows a side branch type resonator typically. It is a figure which shows typically a Helmholtz type resonator.
- (A) is a development view of a part of a tread portion including a stepped resonator
- (b) is a cross-sectional view taken along line AA ′ of the development view shown in (a)
- (c ) Is a cross-sectional view taken along the line BB ′ of the developed view shown in FIG.
- (A) And (b) is a partial expanded view of the tread part of the pneumatic tire of a prior art example.
- (A)-(f) is a partial development view of a tread portion of a pneumatic tire provided with a resonator by the design method according to the present invention.
- FIG. 7 is a diagram showing an optimization region (shaded portion) of air resonance sound of a resonator provided in a pneumatic tire (hereinafter referred to as “tire”) by the design method according to the present invention.
- FIGS. 9A to 9F are development views of a part of a tread portion of a pneumatic tire provided with a resonator by the design method according to the present invention.
- the resonator designing method of the present invention includes at least one circumferential groove 5 extending in the tire circumferential direction on the tread portion tread surface 4, and includes the circumferential groove 5 and the road surface.
- a resonator 1 for reducing noise generated by resonance in the formed pipe is provided, and the resonator 1 extends from the circumferential groove 5 and extends to and from the branch groove portion 2.
- the present invention relates to a method for designing a resonator 1 in a tire including an air chamber portion 3 having a cross-sectional area perpendicular to the direction larger than that of a branch groove portion 2.
- the length of the central axis OO ′ of the branch groove portion 2 is 1, the contact length of the circumferential groove 5 in the ground road surface is L, the portion having the smallest cross-sectional area of the branch groove portion 2 is S min ,
- the position l 1 where the branch groove 2 becomes S min is l 1 / L ⁇ 1 / ⁇ from the opening to the circumferential groove 5, and , L 2 / L ⁇ (l ⁇ l 1 ) / L ⁇ 1 / ⁇
- the relationship between the resonator shape l / L and S min / S max is When,
- the resonator 1 is designed to satisfy the above.
- the circumferential groove 5 is not limited to a straight line shape, and may have other shapes such as a curved line shape and a zigzag shape.
- the volume of the resonator 1 is substantially determined in a region near the end along the axis. Such a volume has the same effect regardless of the position of the resonator 1 close to the end from the position where S min is taken, and the maximum cross-sectional area of the resonator 1 is set as a representative value of the volume in the region. This is S max .
- Equation 6 the frequency obtained from Equation 2 is substituted into Equation 6, It becomes.
- Equation 13 is expanded by Macrolon expansion, Is converted to From this, the following mathematical formula can be derived.
- the resonator designed by this design method from the assumption that ⁇ l 1 / L and ⁇ l 2 / L are sufficiently smaller than 1, It is necessary to satisfy.
- the upper limit formula for determining the hatched portion is in accordance with the constraints of the present design method,
- the lower limit is given by Given in.
- the equation for designing the resonator does not transcend, the shape factor of the resonator can be easily determined, an appropriate resonator can be easily designed, and air column resonance can be effectively performed. It is possible to provide a tire that can reduce noise.
- the resonators 1 are preferably arranged at a plurality of tire circumferential pitches, that is, at so-called variable pitches. This is because when the resonators 1 are all arranged at the same circumferential pitch, the pitch noises of the resonators 1 adjacent to each other in the tire circumferential direction resonate and amplify during tire load rolling. Because there is a possibility of becoming.
- the arrangement pitch of the resonators 1 is smaller than the ground contact length. This is because, when the arrangement pitch of the resonators 1 is larger than the contact length, even if the tire is in contact with the road surface, the resonator 1 does not contact the road surface, and the air column resonance sound is effectively reduced. This is because it may not be possible.
- sipe is a narrow groove having a region in which the cross-sectional area decreases by 90% or more at the time of ground contact, and is not included in the calculation of l and S. At this time, the width of the sipe is preferably 2 mm or less.
- Conventional tires 1 and 2 have tread patterns shown in FIGS. 8A and 8B, respectively, and include a circumferential groove and a conventional resonator that opens in the circumferential groove.
- Each of the tires 1 to 6 has a tread pattern shown in FIGS. 9A to 9F, and includes a circumferential groove and a resonator designed by the design method according to the present invention.
- the depth of all the resonators is 6.5 mm, and each tire has the specifications shown in Table 1.
- Each of these test tires is mounted on a rim of size 7.5J to form a tire wheel, air pressure: 210 kPa (relative pressure), tire load load: 4.0 kN, on an indoor drum tester at 80 km / h.
- air pressure 210 kPa (relative pressure)
- tire load load 4.0 kN
- the evaluation of the air column resonance sound was performed by calculating the volume increasing / decreasing relative to the volume of the noise generated from the conventional tire 1 as a relative value, thereby evaluating the effect of reducing the air column resonance sound. The results are shown in Table 1.
- the tires 1 to 6 of the example tires have reduced air column resonance noise compared to the conventional tires 1 and 2.
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- Engineering & Computer Science (AREA)
- Mechanical Engineering (AREA)
- Tires In General (AREA)
Abstract
Description
すなわち、共鳴器1の軸線長さと主溝長さの比l/Lと、共鳴器の断面積比Smin/Smaxの関係は図7の斜線部分に該当することとなる。なお、ここで斜線部を決定する上限の式は前記の本設計方法の制約に従い、
2 枝溝部
3 気室部
4 トレッド部踏面
5 周方向溝
Claims (2)
- トレッド部踏面に、タイヤ周方向に延びる少なくとも一本の周方向溝を具え、該周方向溝と路面とで形成される管内の共鳴により発生する騒音を低減するための共鳴器を有し、該共鳴器は、該周方向溝から分岐して延びる枝溝部及び、該枝溝部につながり、延在方向に直交する断面の面積が該枝溝部のそれよりも大きい気室部を具える空気入りタイヤの共鳴器の設計方法において、
前記枝溝部の中心軸O-O’の長さをl、前記周方向溝の接地路面内における接地長をL、該枝溝部の最も断面積が小さい部分をSmin、前記気室部の断面積の最も大きい部分をSmaxとしたとき、枝溝部がSminとなる位置l1が周方向溝への開口部よりl1/L<1/πであり、且つ、l2/L<(l-l1)/L<1/πであり、かつ、共鳴器の形状l/Lと、Smin/Smaxの関係が、
となるよう共鳴器を設計することを特徴とする共鳴器の設計方法。 - トレッド部踏面に、タイヤ周方向に延びる少なくとも一本の周方向溝を具え、該周方向溝と路面とで形成される管内の共鳴により発生する騒音を低減するための共鳴器を有し、該共鳴器は、該周方向溝から分岐して延びる枝溝部及び、該枝溝部につながり、延在方向に直交する断面の面積が該枝溝部のそれよりも大きい気室部を具える空気入りタイヤにおいて、
前記枝溝部の中心軸O-O’の長さをl、前記周方向溝の接地路面内における接地長をL、該枝溝部の最も断面積が小さい部分をSmin、前記気室部の断面積の最も大きい部分をSmaxとしたとき、枝溝部がSminとなる位置l1が周方向溝への開口部よりl1/L<1/πであり、且つ、l2/L<(l-l1)/L<1/πであり、かつ、共鳴器の形状l/Lと、Smin/Smaxの関係が、
を満たすことを特徴とする空気入りタイヤ。
Priority Applications (4)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
US13/322,011 US20120067479A1 (en) | 2009-05-28 | 2010-05-08 | Method of designing resonator and pneumatic tire having the resonator |
KR1020117028126A KR101311593B1 (ko) | 2009-05-28 | 2010-05-28 | 공명기의 설계 방법 및 공명기를 구비하는 공기 타이어 |
CN2010800234409A CN102448742A (zh) | 2009-05-28 | 2010-05-28 | 共鸣器的设计方法和具有该共鸣器的充气轮胎 |
EP10780305.8A EP2436534B1 (en) | 2009-05-28 | 2010-05-28 | A method of designing a resonator and pneumatic tire having the resonator |
Applications Claiming Priority (2)
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JP2009-129469 | 2009-05-28 | ||
JP2009129469A JP5255520B2 (ja) | 2009-05-28 | 2009-05-28 | 空気入りタイヤ |
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WO2010137345A1 true WO2010137345A1 (ja) | 2010-12-02 |
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PCT/JP2010/003615 WO2010137345A1 (ja) | 2009-05-28 | 2010-05-28 | 共鳴器の設計方法及び共鳴器を具える空気入りタイヤ |
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US (1) | US20120067479A1 (ja) |
EP (1) | EP2436534B1 (ja) |
JP (1) | JP5255520B2 (ja) |
KR (1) | KR101311593B1 (ja) |
CN (1) | CN102448742A (ja) |
WO (1) | WO2010137345A1 (ja) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP2465707A1 (en) * | 2010-12-14 | 2012-06-20 | Toyo Tire & Rubber Co. Ltd. | Pneumatic tire |
Families Citing this family (7)
Publication number | Priority date | Publication date | Assignee | Title |
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JP5231405B2 (ja) * | 2007-05-14 | 2013-07-10 | 株式会社ブリヂストン | 空気入りタイヤ |
JP6166913B2 (ja) | 2013-02-28 | 2017-07-19 | 株式会社ブリヂストン | 空気入りタイヤ |
JP5852167B2 (ja) | 2014-04-04 | 2016-02-03 | 株式会社ブリヂストン | タイヤ |
WO2019117090A1 (ja) * | 2017-12-13 | 2019-06-20 | 株式会社ブリヂストン | 空気入りタイヤ |
JP7139288B2 (ja) * | 2019-06-11 | 2022-09-20 | 株式会社ブリヂストン | タイヤ |
EP4147884A4 (en) * | 2020-05-08 | 2023-11-22 | Bridgestone Corporation | TIRES |
EP4147883A4 (en) * | 2020-05-08 | 2023-11-22 | Bridgestone Corporation | TIRES |
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WO2004103737A1 (ja) | 2003-05-21 | 2004-12-02 | Bridgestone Corporation | 空気入りタイヤおよびそのタイヤのトレッドパターンの設計方法 |
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JP2008179289A (ja) | 2007-01-25 | 2008-08-07 | Bridgestone Corp | 空気入りタイヤ |
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JP2009090824A (ja) * | 2007-10-09 | 2009-04-30 | Bridgestone Corp | 空気入りタイヤ |
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CN101360619B (zh) * | 2005-12-21 | 2010-05-19 | 株式会社普利司通 | 充气轮胎 |
JP5366539B2 (ja) * | 2006-03-31 | 2013-12-11 | 株式会社ブリヂストン | 空気入りタイヤ |
CN101663176B (zh) * | 2007-02-19 | 2012-02-08 | 株式会社普利司通 | 充气轮胎 |
-
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- 2009-05-28 JP JP2009129469A patent/JP5255520B2/ja not_active Expired - Fee Related
-
2010
- 2010-05-08 US US13/322,011 patent/US20120067479A1/en not_active Abandoned
- 2010-05-28 KR KR1020117028126A patent/KR101311593B1/ko active IP Right Grant
- 2010-05-28 CN CN2010800234409A patent/CN102448742A/zh active Pending
- 2010-05-28 WO PCT/JP2010/003615 patent/WO2010137345A1/ja active Application Filing
- 2010-05-28 EP EP10780305.8A patent/EP2436534B1/en not_active Not-in-force
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WO2004103737A1 (ja) | 2003-05-21 | 2004-12-02 | Bridgestone Corporation | 空気入りタイヤおよびそのタイヤのトレッドパターンの設計方法 |
JP2007237751A (ja) | 2006-03-03 | 2007-09-20 | Bridgestone Corp | タイヤ性能予測方法、タイヤ設計方法及びプログラム |
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JP2008179289A (ja) | 2007-01-25 | 2008-08-07 | Bridgestone Corp | 空気入りタイヤ |
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Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP2465707A1 (en) * | 2010-12-14 | 2012-06-20 | Toyo Tire & Rubber Co. Ltd. | Pneumatic tire |
US8708010B2 (en) | 2010-12-14 | 2014-04-29 | Toyo Tire & Rubber Co., Ltd. | Pneumatic tire |
Also Published As
Publication number | Publication date |
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EP2436534A1 (en) | 2012-04-04 |
JP5255520B2 (ja) | 2013-08-07 |
EP2436534B1 (en) | 2014-06-04 |
US20120067479A1 (en) | 2012-03-22 |
KR101311593B1 (ko) | 2013-09-26 |
EP2436534A4 (en) | 2013-04-17 |
CN102448742A (zh) | 2012-05-09 |
KR20120023020A (ko) | 2012-03-12 |
JP2010274787A (ja) | 2010-12-09 |
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