1. Technical Field
The invention relates to a disc brake for a heavy vehicle comprising a disc brake having a disc-shaped rotor consisting of a cast iron alloy and a calliper supporting a brake lining which is intended to be pressed against the said rotor during braking. More particularly, the invention relates to disc brakes intended to absorb a braking torque equal to and greater than 12 kNm, especially a braking torque between 12 and 25 kNm. These brakes are intended for heavy vehicles, by which is meant vehicles having an axle pressure in excess of 5 tons, especially vehicles having an axle pressure between 6 and 14 tons.
2. Background Art
Disc brakes are being used more and more frequently for heavy vehicles. A distinction can be drawn between two types of disc brakes for heavy vehicles, firstly hat-shaped brake discs in which a disc with radial extent is configured with a centrally situated, axially running cylindrical protrusion intended for fastening to a wheel axle, and secondly brake discs which are substantially symmetrical with respect to a plane running at right angles through the rotational axis of the brake disc and have a central bushing intended for fastening to a wheel hub. One problem with hat-shaped brake discs is that the brake disc is not supported symmetrically with respect to a plane running at right angles through the rotational axis of the brake disc, which means that the disc slants when it is heated. The effect of this is that the pressure from the brake lining is not evenly distributed over the brake, so that the brake disc is at greater risk of cracking. In order to reduce the risk of disc fracture, brake discs have therefore been produced which are substantially symmetrical with respect to a plane running at right angles through the rotational axis of the brake disc and which have a central bushing intended for fastening to a wheel hub. Such a brake disc is shown in EP 621 829. The bearing surfaces of these discs remain flat during heating, so that the pressure from the brake linings is more advantageously distributed and the risk of cracking is reduced.
A further problem with the use of brake discs is the occurrence of bandwear. Band-shaped wear is a phenomenon which occurs as a result of the contact surface between lining and rotor not being completely flat. This phenomenon is explained in greater detail below in connection with
The presence of bands gives rise to the formation of local plasticized zones, thereby producing an increased risk of cracking. The successive formation of bands to and fro between central and peripheral regions of the disc further gives rise to the risk of fatigue failure as a result of the constantly occurring load change. It has been shown that the band can move one or more times between outer edges and central sections of the disc, even during one and the same braking cycle.
One object of the invention is to provide a brake disc offering reduced occurrence of disc cracking. Another object of the invention is to provide a brake disc in which the frequency of change between different band modes is reduced.
The said objects of the invention are achieved according to a first embodiment of the invention having a brake disc according to the characterizing part of patent claims 1 and 9.
To aid understanding of the invention, the following theoretical background is provided: Trials have been conducted involving brake tests in a test bench for brake discs and brake linings of different proportions. Observations show that brake linings having a small radial extent, B, are less prone to cracking. An explanation of this is that the relationship between the width of the brake lining, from the inner edge of the brake lining in the radial extent to the outer edge of the brake lining in the radial extent, and a contact band formed owing to the irregularity of both disc and lining is more advantageous. This means that for a certain level of energy input to the disc brake, there is an optimal relationship between the width of the said contact or wear band w and the radial extent B of the brake lining. By radial extent is here meant the distance from the inner edge of the brake lining in the radial extent to the outer edge.
We introduce a relationship γ=B/R, in which B is constituted by the radial extent of the brake lining and R is the radius of the disc. In the tests which γ have been conducted, γ=0.42 for the wide lining and γ=0.37 for the narrow lining. The test showed that the narrow lining obtained a 33% longer working life, despite the fact that the disc was 3.8 kg lighter, which is negative from the cracking aspect since the disc becomes warmer.
The test shows that the occurrence of disc cracking can partially be explained by the aforementioned phenomenon of band-shaped wear. Cracks are formed as a result of the stresses which arise in respect of each separate band mode which occurs within the extent of the brake lining means. Usually a central mode is formed when wear occurs in a centrally situated band and a peripheral mode when wear occurs close to the edges of the lining. These stresses from these two modes are oppositely directed and therefore give rise to a load which alternates in direction. The changes of mode can arise even during a long braking cycle. The risk of fatigue failure is therefore high. One object of the invention is therefore to reduce the width of the brake lining means such that the likelihood of two separate brake modes arising is lessened. If the radial extent of the lining is of the same order of magnitude as the band, the risk of occurrence of two separate band modes is reduced. If, on the other hand, the radial extent of the brake lining means is too small, the wear on the lining means and the disc brake means will become too great, adversely affecting the working life.
One object of the invention is therefore to reduce the occurrence of cracking on the brake discs. This is performed by reducing the likelihood of bandwear occurring in a plurality of modes. This is achieved by maximizing the width of the band-shaped wear zone in relation to the radial extent B of the brake lining. Maximizing the width w of the band-shaped wear zone is equivalent to maximizing the time derivative of the width. We therefore have the following two equations:
max (w/B) 1)
max ((δw/δt)/B) 2)
The width w of the band-shaped wear zone is dependent on the following material parameters: the E modulus of the lining, thermal expansion of lining and disc, thermal conduction of lining and disc and wear resistance of lining and disc. These parameters are kept constant during the following analysis, in which the geometric characteristics of lining and disc are investigated.
For a given material, the width w of the band-shaped wear zone is a function of supplied energy to the disc brake at a given radius of the brake disc. The analysis makes use of the following two hypotheses:
The rate of growth of the band is proportional to the power input:
δw/δt˜P H1)
The rate of growth of the active area Aact in which contact exists between lining and brake disc is proportional to the power
δAact/δt˜P H2)
We have the following relationship between active area and the band width
Aact=2πrw 3)
We thus obtain the following:
δAact/δt=2πrδw/δt 4)
Which means that
δw/δt˜P/R 5)
As a consequence of the above-stated hypotheses, we obtain, together with equation 2), max(δw/δt)/B) and hypothesis H1, if brake power is constant:
max(1/B) 6)
Together with hypothesis H2, we obtain
max(1/RB). 7)
The analysis therefore reveals that, in order to obtain a minimal risk of occurrence of changes between band modes, according to hypothesis H1 the radial extent B of the lining should be made as small as possible and, for hypothesis H2, the radial extent B of the lining and the radius R of the brake disc should be made as small as possible.
Brake discs are configured so as to be able to absorb and carry off the heat which is generated in braking. This means that the volume of the brake disc is substantially proportional to the axle pressure of the vehicle. This means that smaller discs are required for lower axle pressure and that the width w of the band-shaped wear zone decreases for reduced axle pressure.
The invention will be described in greater detail below with reference to the appended figures of the drawing, in which:
a shows in diagrammatic representation the cross section of a brake disc and a brake lining having perfectly flat surfaces,
b shows in diagrammatic representation the cross section of a brake disc and a brake lining having an irregularity in which initial contact takes place,
c shows in diagrammatic representation the growth of the irregularity during thermal expansion of disc and lining,
d shows in diagrammatic representation a band-shaped, wornregion of the irregularity,
In
The brake disc has an active diameter D, which stretches from the centre of the brake disc to the point of contact between lining and brake disc lying at the greatest distance from the said centre. The brake lining has a radial extent B, which is the distance from the points of contact between lining and disc lying closest to the centre to those lying farthest from the centre. In determining the radial extent B of the brake lining, this measurement is defined as the mean value of the distance between the inner and outer radial periphery 36, 37 of the lining along 50% of the extent of the brake lining in the angular direction φ.
Instead of fixing the brake disc to the hub by screwing the disc to a flange on the hub, as has hitherto been the norm, in the construction according to the embodiment shown in
As can especially be seen from
In the embodiment shown in
As can be seen from
For heavy vehicles, it has been shown that the following measures of the radial extent are suitable for suppressing the formation of band-shaped wear zones in a plurality of modes:
It has also been shown that for heavy vehicles, i.e. for vehicles having a braking torque between 12-25 kNm and/or an axle pressure between 6 14 tons, the relationship between the radial extent of the brake lining and the radius R of the brake disc B/R should be less than 0.38.
The brake discs are expediently sized according to the following table:
According to a standard brake discs construction, the weight of the brake disc should be proportional to the axle load.
The brake lining is preferably configured in a rigid material having a tangential modulus of elasticity E=600 Mpa, at a contact pressure of 2 MPa and at room temperature, for brake discs intended for a braking torque of 20-25 kNm; a tangential modulus of elasticity E=500 Mpa, at a contact pressure of 2 MPa and at room temperature, for brake discs intended for a braking torque of 16-20 kNm; and a tangential modulus of elasticity E=400 Mpa, at a contact pressure of 2 MPa and at room temperature, for brake discs intended for a braking torque of 12-16 kNm.
The brake discs preferably have a diameter greater than 370 mm.
The brake discs are preferably made from a material having the following properties:
The brakes are configured with disc weights according to the table below in order to reach a temperature of less than 700° C. during a 40 s long braking cycle at a vehicle speed of 85 km/h.
The invention should not be limited to the above-specified embodiments but is appropriate for use in connection with disc brakes of a wide variety of types, for example in connection with such brake discs in which the centre of the rotor is fastened to the wheel axle by an axially running cylindrical protrusion, i.e. a top-hat-shaped brake disc.
Number | Date | Country | Kind |
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0101252 | Apr 2001 | SE | national |
The present application is a continuation patent application of International Application No. PCT/SE02/00698 filed 9 Apr. 2002 which was published in English pursuant to Article 21(2) of the Patent Cooperation Treaty, and which claims priority to Swedish Application No. 0101252-5 filed 10 Apr. 2001. Both applications are expressly incorporated herein by reference in their entireties.
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Number | Date | Country | |
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20040129509 A1 | Jul 2004 | US |
Number | Date | Country | |
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Parent | PCT/SE02/00698 | Apr 2002 | US |
Child | 10605598 | US |