Disk rotor of vehicle brake
11549561 · 2023-01-10
Assignee
Inventors
- Yoji Kawamoto (Aki-gun, JP)
- Natsumi Sato (Aki-gun, JP)
- Shunsaku Shibata (Aki-gun, JP)
- Tomoki Nakayama (Aki-gun, JP)
- Shoji Goto (Aki-gun, JP)
- Yuki Ikawa (Aki-gun, JP)
- Kentaro Ota (Aki-gun, JP)
Cpc classification
F16D2055/0037
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F16D2065/1384
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F16D65/0081
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F16D65/128
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F16D2065/1316
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F16D2065/1328
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F16D2065/132
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F16D2065/1324
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F16D65/127
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
International classification
Abstract
A disk rotor of a vehicle brake with improved efficiency in cooling the disk rotor by a synergy effect that comes from ensuring velocity of airflow flowing between cooling fins, ensuring surface areas of the cooling fins, and generating turbulent flow by second fins. A plurality of cooling fins each extending radially from an inner peripheral edge to an outer peripheral edge of a disk rotor are provided inside the disk rotor at intervals in the circumferential direction. Each of the plurality of the cooling fins includes a radial fin extending radially and a second fin spaced apart from the radial fin in the radial direction.
Claims
1. A disk rotor of a vehicle brake comprising: a plurality of cooling fins provided inside the disk rotor at intervals in a circumferential direction, each extending radially from a region proximal an inner peripheral edge of the disk rotor to a region proximal an outer peripheral edge of the disk rotor, wherein each of the plurality of cooling fins includes a radial fin extending radially and a plurality of second fins extending radially, spaced apart from the radial fin, and aligned with the radial fin in a radial direction of the disk rotor, the plurality of second fins has a shorter length than the radial fin in the radial direction of the disk rotor, the radial fin is provided on an inner periphery side of the disk rotor, and the plurality of second fins is provided on an outer periphery side of the disk rotor, the radial fin is provided over a half or more of a length of the disk rotor in the radial direction thereof, between circumferentially adjacent two of the plurality of cooling fins, a third fin is provided only on an outer peripheral half of the disk rotor between the radial fin and the plurality of second fins in the radial direction and between two fins of the plurality of second fins in the radial direction, and inner and outer edges of the third fin radially overlap edges of the radial fin and one of the plurality of the second fins adjacent to each other in the radial direction.
2. The disk rotor of a vehicle brake according to claim 1, wherein the radial fin is composed of an oval fin having an oval shape.
3. The disk rotor of a vehicle brake according to claim 2, wherein the plurality of second fins have a perfect or approximately perfect circular shape and are provided in a direction extending from the oval fin.
4. The disk rotor of a vehicle brake according to claim 3, wherein a total of outer peripheral areas of the oval fin, the second fins, and the third fin are larger than an outer peripheral area of a cooling fin that is formed of a single radial fin alone.
5. The disk rotor of a vehicle brake according to claim 2, wherein a total of outer peripheral areas of the oval fin, the second fins, and the third fin are larger than an outer peripheral area of a cooling fin that is formed of a single radial fin alone.
Description
BRIEF DESCRIPTION OF THE DRAWINGS
(1)
(2)
(3)
(4)
(5)
(6)
(7)
(8)
(9)
(10)
(11)
DETAILED DESCRIPTION
(12) Accordingly, improving efficiency in cooling the disk rotor by a synergy effect that comes from ensuring velocity of airflow flowing between the cooling fins, ensuring surface areas of the cooling fins, and generating turbulent flow by the second fins has been accomplished with a disk rotor of a vehicle brake including a plurality of cooling fins arranged inside the disk rotor at intervals in a circumferential direction and each extending radially from an inner peripheral edge to an outer peripheral edge of the disk rotor. Each of the plurality of cooling fins includes a radial fin extending radially and a second fin spaced apart from the radial fin in a radial direction.
EXAMPLES
(13) An example of this disclosure will be detailed below with reference to the drawings. The drawings illustrate a disk rotor of a vehicle brake, wherein
(14) While the disk rotor of the vehicle brake of the present disclosure may be used in any of left and right front wheels and left and right rear wheels, examples given below describe a structure in which the disk rotor is used in a left front wheel of a vehicle. In
(15) A wheel assembly 4 is disposed in the wheel well 3. As shown in
(16) As shown in
(17) As shown in
(18) As shown in
(19) As shown in
(20) As shown in
(21) As shown in
(22) In other words, all of the disk portion 5D of the wheel 5, the flange portion 7b of the hub 7, and the disk rotor 20 are co-fastened and fixed by the fastening members 19 shown in
(23) As shown in
(24) The hat portion 20a, the outer sliding face 20b, and the inner sliding face 20c are integrally formed by sand casting. Both of the outer sliding face 20b and the inner sliding face 20c constitute a ventilated disk.
(25) As shown in
(26) As shown in
(27) As shown in
(28) Also, as shown in
(29) As shown in
(30) As shown in
(31) As shown in
(32) As shown in
(33) These openings 32, 33, and 34 are openings for cooling the disk rotor 20 by taking in traveling air to the inner peripheral surface of the disk rotor 20, more specifically, between the inner sliding face 20c and the outer sliding face 20b. As shown in
(34) As shown in
(35) As shown in
(36) The beads 30a, 30b, 30c, 30d, and 30e helps increase rigidity of the dust cover 30. It should be noted that for convenience of illustration, the beads 30a, 30b, 30c, 30d, and 30e have been omitted in
(37) As shown in
(38) The clearance CL is set in the range from 8 to 15 mm That is, the following are the results of computational fluid dynamics (CED) analysis carried out under conditions in which the clearance CL between the dust cover 30 and the rim portion 5R of the wheel 5 is 22 mm, 10 mm, and 0 mm.
(39) Taking the ratio of the heat transfer coefficient h when the CL=22 mm as 100%, the ratio when the CL=10 mm was 103%, and the ratio when the CL=0 mm was 110%.
(40) That is, reducing the clearance CL from 22 mm to 10 mm results in a 3% improvement in the heat transfer coefficient, and reducing the clearance CL from 22 mm to 0 mm results in a 10% improvement in the heat transfer coefficient.
(41) The upper limit of the clearance CL is set to 15 mm or less for good performance of the heat transfer coefficient h. The lower limit of the clearance CL is set to 8 mm taking into account productivity. If the clearance CL is less than 8 mm, the outer peripheral edge of the dust cover 30 may interfere with the rim portion 5R due to production variation. Accordingly, the clearance CL is set in the range from 8 to 15 mm.
(42) Bringing the outer peripheral edge of the dust cover 30 close to the inner peripheral surface of the rim portion 5R of the wheel 5 as shown in
(43) As the openings 32, 33, and 34 are provided in the dust cover 30 positioned on the inner face side of the disk rotor 20 in the vehicle width direction, the openings 32, 33, and 34 can be positioned in the positive pressure area α and the outer peripheral portion of the disk rotor 20 can be positioned in the negative pressure area β.
(44) Pressure difference between the above positive pressure and negative pressure improves the airflow velocity, which helps improve efficiency in cooling the disk rotor 20. Specifically, traveling air having entered the vehicle-width-direction inner side of the dust cover 30 inside the wheel 5 through a portion below the bumper from the vehicle front side then enters in between the inner sliding face 20c and the outer sliding face 20b from the openings 32, 33, and 34 of the dust cover 30 as shown by arrows in
(45) As shown by the arrows in
(46) In
(47)
(48) In the example (Example 1) shown in
(49) Each of the multiple cooling fins 40 includes a radial fin 41 that extends radially and multiple (two in this example) second fins 42, 42 for generating turbulent flow that are spaced apart from the radial fin 41 by a gap g in the radial direction.
(50) As shown in
(51) Splitting each cooling fin 40 into the radial fin 41 and the second fins 42 in this manner helps more efficiently cool the disk rotor 20 by the synergy effect that comes from ensuring the velocity of airflow flowing between the circumferentially adjacent cooling fins 40, 40, ensuring fin surface areas, and generating turbulent flow by the second fins 42.
(52) In particular, turbulent flow is generated by the second fins 42. The heat transfer coefficient of this turbulent flow is significantly larger than that of laminar flow, thereby helping improve efficiency in cooling the disk rotor 20.
(53) As shown in
(54) Positioning the oval fin (radial fin 41) on the inner periphery side in this manner helps improve airflow velocity by virtue of mutual pumping performance by circumferentially adjacent oval fins (radial fins 41, 41), and this airflow with improved velocity brings about turbulent flow at the second fins 42.
(55) Additionally, as shown in
(56) Making the oval fin (radial fin 41) as long as, or longer than, a half of the disk rotor 20 in the radial direction thereof in this manner ensures sufficient pumping performance, which in turn allows obtaining sufficient airflow velocity. This helps further improves efficiency in cooling the disk rotor 20 by the synergy effect that comes from ensuring this airflow velocity, ensuring the surface area by the oval fin (radial fin 41) and the second fins 42, and generating turbulent flow by the multiple second fins 42.
(57) In this example, as shown in
(58) Additionally, as shown in
(59) Providing the third fins 43 compensates for decrease in brake surface pressure during braking at the gaps between the radially extending oval fin (radial fin 41) and the second fin 42 and between the inner and outer second fins 42, 42. Additionally, increasing the outer peripheral surface areas helps further improve the efficiency in cooling the disk rotor 20. Additionally, turbulent flow is also generated by the third fins 43, thereby helping further improve the heat transfer coefficient.
(60) As shown in
(61) As shown in
(62) In short, as shown in
(63)
(64) The example shown in
(65) The disk rotor of the vehicle brake of Example 2 shown in
(66) In the comparative example, an opening angle θ2 between circumferentially adjacent cooling fins 50, 50 is made smaller than the opening angle θ1 in Examples 1 and 2. That is, a relational expression of θ2<θ1 holds. In
(67)
h∝Nu [Expression 1]
(68) Herein, Nu denotes the Nusselt number, which is a dimensionless number (a quantity whose value is independent of units) representing the magnitude of the heat transfer coefficient h. Specifically, the Nusselt number Nu is a dimensionless number given by the ratio of heat capacity transferred by heat convection during flow of a fluid to heat capacity considered to be transferred by heat conduction alone while the fluid is stationary.
(69) The Nusselt number Nu becomes larger when the traveling air flowing through the ventilation hole 44 is turbulent flow than when it is laminar flow. In other words, the magnitude of the heat transfer coefficient h depends on whether the traveling air is laminar flow or turbulent flow, and the heat transfer coefficient h has a larger value when the traveling air is turbulent flow. The Nusselt number Nu when the traveling air is laminar flow can be expressed by the following Expression 2, and the Nusselt number Nu when the traveling air is turbulent flow can be expressed by the following Expression 3.
(70)
(71) Herein, Re denotes the Reynolds number, and Pr denotes the Prandtl number. Specifically, the Reynolds number Re is a dimensionless number representing a ratio of viscous forces to inertial forces of flow; at lower Reynolds number Re than a certain value, laminar flow takes place that flows smoothly, and at higher Reynolds number Re than a certain value, turbulent flow takes place that contains irregular fluctuating components in its speed and pressure.
(72) The Prandtl number Pr is the ratio of momentum energy diffusion rate to thermal energy diffusion rate. That is, the Prandtl number Pr is a dimensionless number defined by the ratio of kinematic viscosity coefficient, which is a momentum diffusion coefficient, to thermal diffusion coefficient. The Prandtl number Pr is a physical property value intrinsic to fluids, and the Prandtl number Pr of air is 0.7. Further, a radiation amount Q representing an effect of an improvement in cooling can be expressed by the following Expression 4.
Q=h×A×ΔT [Expression 4]
(73) Herein, h denotes the heat transfer coefficient, A denotes the surface area (the total of outer peripheral surface areas of all fins), and ΔT denotes a difference between temperature of the disk rotor 20 and atmospheric temperature (i.e., outside temperature).
(74) The fin structure of the comparative example shown in
(75) In addition to the second fins 42, 42, the fin structure of Example 1 shown in
(76) In regard to the surface area A, which affected the radiation amount Q, when the surface area A of the comparative example was defined as 100%, Example 2 had a similar surface area. That is, in Example 2, while the surface areas of the fins 41, 42 decreased as a function of the width W and the gaps between the fins 41, 42 and between the fins 42, 42, surfaces areas of both inner and outer faces of ventilating portions in the vehicle width direction corresponding to the gaps between the fins 41, 42 and between the fins 42, 42 increased, resulting in a similar surface area to that of the comparative example. The fin structure of Example 1 shown in
(77) In regard to the cooling efficiency expressed by the product of the heat transfer coefficient h and the surface area A (h×A), when the cooling efficiency of the comparative example shown in
(78) As described above, the disk rotor of the vehicle brake of the above examples includes multiple cooling fins 40 provided inside the disk rotor 20 (more specifically, between the outer sliding face 20b and the inner sliding face 20c) at intervals in the circumferential direction and extending radially from the inner peripheral edge to the outer peripheral edge of the disk rotor 20, and each of the multiple cooling fins 40 includes a radial fin 41 extending radially, and the second fins 42 spaced apart from the radial fin 41 by the gap g in the radial direction (see
(79) With this configuration, each cooling fin 40 is split into the radial fin 41 and the second fins 42, and this helps more efficiently cool the disk rotor 20 by the synergy effect that comes from ensuring the velocity of airflow flowing between the circumferentially adjacent cooling fins 40, 40, ensuring fin surface areas, and generating turbulent flow by the second fins 42. In particular, turbulent flow can be generated by the second fins 42. The heat transfer coefficient h of this turbulent flow (see
(80) In one embodiment of this disclosure, the radial fin 41 is composed of an oval fin having an oval shape, and each of the second fins 42 is formed with a shorter length than that of the oval fin (radial fin 41) in the radial direction of the disk rotor 20. The oval fin (radial fin 41) is positioned on the inner periphery side of the disk rotor 20, and the second fins 42 are positioned on the outer periphery side of the disk rotor 20 (see
(81) With this configuration, pumping performance by the oval fins (radial fins 41) positioned on the inner periphery side of the disk rotor 20 (more specifically, on the inner periphery side between the outer sliding face 20b and the inner sliding face 20c) helps improve the airflow velocity, and this airflow with improved velocity can bring about turbulent flow at the second fins 42.
(82) In one embodiment of this disclosure, the oval fin (radial fin 41) is provided over a half or more of the length of the disk rotor 20 in the radial direction thereof, and the multiple second fins 42 having a perfect or approximately perfect circular shape are provided in a direction extending from the oval fin (radial fin 41) (see
(83) With this configuration, the oval fin (radial fin 41) is made as long as, or longer than, a half of the disk rotor 20 in the radial direction thereof (more specifically, in the radial direction of the sliding faces 20b, 20c), and this allows obtaining sufficient pumping performance, thereby helping ensure sufficient airflow velocity.
(84) This helps further improve the efficiency in cooling the disk rotor 20 (see h×A in
(85) Additionally, in one embodiment of this disclosure, between circumferentially adjacent cooling fins 40, 40, the third fin 43 is provided at least one of between the oval fin (radial fin 41) and the second fin 42 and between the multiple second fins 42, 42, and a total of outer peripheral areas of the oval fin (radial fin 41), the second fins 42, 42, and the third fin 43 are made larger than an outer peripheral area of a cooling fin when it is formed of a single radial fin alone (see
(86) With this configuration, the third fin 43 can compensate for decrease in brake surface pressure at the gap between the radially extending oval fin (radial fin 41) and the second fin 42 or between the second fins 42, 42. Also, increase in the outer peripheral surface area (see the surface area A in
(87) Additionally, in one embodiment of this disclosure, as viewed in the circumferential direction, inner and outer edges of the third fin 43 radially overlap edges of the oval fin (radial fin 41) and the second fin 42 adjacent to each other in the radial direction (see
(88) As regards correspondence between the configuration of this disclosure and the above examples, the inside of the disk rotor 20 of this disclosure corresponds to the portion between the outer sliding face 20b and the inner sliding face 20c in the examples, and likewise, the oval fin corresponds to the radial fin 41. However, this disclosure is not limited only to the configuration of the above examples.
(89) For example, while in the above examples the fins 41, 42, and 42 are arranged linearly in the radial direction, instead of this structure, the fins 41, 42, and 42 may be arranged along a virtual curved line that extends radially in a curved manner from the inner to outer peripheral edges of the disk rotor 20.
(90) As described above, the present disclosure is useful for a disk rotor of a vehicle brake including multiple cooling fins provided inside the disk rotor at intervals in the circumferential direction and each extending radially from inner to outer peripheral edges of the disk rotor.