The present invention relates to a method for the indirect tire pressure monitoring in which an analysis of the natural oscillation behavior of at least one tire is performed and at least one pressure loss analysis variable (fFL, fFR, fRL, fRR), in particular a natural frequency, is determined, in which case a temperature compensation (4) of the pressure loss analysis variable (fFL, fFR, fRL, fRR) is performed, and to a computer program product.
In up-to-date motor vehicles, systems are employed at an increasing rate, which contribute to an active or passive protection of the occupants. Systems for tire pressure monitoring protect the occupants of a vehicle against vehicle damages, which are due to an incorrect tire inflation pressure, for example. An abnormal tire inflation pressure can also cause increase of e.g. tire wear and fuel consumption, or a tire defect (tire bursting) may occur. Various tire pressure monitoring systems are known, which operate either based on directly measuring sensors or detect an abnormal tire pressure by evaluating rotational speed properties or oscillating properties of the vehicle wheels.
German patent application DE 100 58 140 A1 discloses a so-called indirectly measuring tire pressure monitoring system (DDS: Deflation Detection System) detecting tire pressure loss by evaluating the rotational movement of the wheel.
EP 0 578 826 B1 discloses a device for determining tire pressure which determines pressure loss in a tire based on tire oscillations.
EP 0 895 880 A2 discloses a device for estimating the inflation pressure of a tire which comprises a temperature sensor measuring the temperature of the outside air. Effects of the temperature on the resonance frequency of the tire are corrected based on the defined outside air temperature.
An object of the invention is to provide a tire pressure monitoring system for a motor vehicle based on the evaluation of the tire oscillations, in which the influence of the temperature is taken into consideration.
According to the invention, this object is achieved by the method for the indirect tire pressure monitoring in which an analysis of the natural oscillation behavior of at least one tire is performed and at least one pressure loss analysis variable (fFL, fFR, fRL, fRR), in particular a natural frequency, is determined, in which case a temperature compensation (4) of the pressure loss analysis variable (fFL, fFR, fRL, fRR) is performed. A tire temperature (Ttire) calculated by means of a temperature model (1) is used to determine a compensation quantity (2), in particular the quotient of variation of the pressure loss analysis variable and change in temperature.
The invention is based on the idea of determining a compensation quantity for at least one pressure loss analysis variable which is obtained by analysis of the torsion natural oscillation behavior of at least one tire. This compensation quantity depends on a tire temperature calculated by means of a temperature model.
It is preferred to use a quotient of a variation of the pressure loss analysis variable to a change in temperature for the compensation quantity. The quotient reflects directly the influence of the temperature on the pressure loss analysis variable.
It is likewise preferred that one compensation quantity is determined for each pressure loss analysis variable. This renders an individual correction of each pressure loss analysis variable possible.
The pressure loss analysis variable preferably concerns a natural frequency or natural frequency shift determined in a natural frequency analysis.
It is, however, also preferred that the pressure loss analysis quantity is a quantity which is obtained from the frequency shift and additional quantities that describe spectra, or a spring constant describing the tire.
According to a preferred embodiment, the temperature model employed considers at least one of the following changes in the quantity of heat in order to calculate the tire temperature: heat flow due to the flexing energy of the tire ({dot over (Q)}Walk), heat flow due to convection ({dot over (Q)}Convection), heat flow due to radiation of the tire ({dot over (Q)}Radiation), heat flow due to heat input of the vehicle ({dot over (Q)}VehicleCondition).
In an improvement of the invention, the compensation quantity/quantities is/are learnt, in which case the pressure loss analysis variable(s) is(are) considered together with the calculated tire temperature(s) over one or more travels in order to learn the compensation quantity/quantities. The learning operation over a long period allows safeguarding sufficient statistical relevance of the result.
Preferably, the tire temperature is determined by integration with time from the at least one change in the quantity of heat. With particular preference, the tire temperature is determined by integration of all changes in the quantity of heat.
In order to calculate the tire temperature, at least two of the following quantities are taken into consideration: outside temperature (Toutside), temperature in a control unit, engine air intake temperature, coolant temperature, engine temperature (Tengine), brake temperature (Tbrake), immobilization time of the vehicle, driving profile since the ignition has been switched on, especially vehicle speed (v), yaw rate, lateral acceleration, drive torque and/or kilometers traveled, ambient sensor information, in particular rain sensor information and/or dew point sensor information.
One advantage of the method of the invention can be seen in the reduced danger of false alarms or the danger of the absence of alarms when pressure loss occurs.
The invention also relates to a computer program product which defines an algorithm according to the method described hereinabove.
Further preferred embodiments can be seen in the following description by way of the Figures.
In the accompanying drawings,
The tire temperature has an influence on the pressure in the tire. Following a raised tire temperature is an increase in tire pressure, hence, an increased rigidity of the tire and an increase in natural frequency. However, the rigidity of the tire material (rubber) is also influenced by the temperature. Ensuing from an increase in temperature is softer rubber, hence, a reduced rigidity and a reduction in natural frequency. It has proved that the two effects do not counterbalance each other in their influence on the tire and, thus, preferably on the natural frequency, but that the effect depends on material, tire temperature and internal pressure. During travels with high temperature variations, this causes changes of the torsion oscillation behavior of a tire which lie in the size range of the changes during pressure loss, what is accompanied by an increased danger of false alarms or the risk of no alarms during pressure loss.
The method of the invention is used in a system for the indirect monitoring of tire pressure in which an analysis of the natural oscillation behavior or one or more tires is performed. As this occurs, a pressure loss analysis variable is determined for at least one tire, preferably for each tire. The natural frequency shift f from the frequency analysis is used in the following description as an example for a pressure loss analysis variable. This is, however, also possible with a pressure loss analysis variable which results from the frequency shift and further quantities that describe spectra, as is e.g. described in detail in publication WO 2005/005174 A1, or likewise with a spring constant of the tire, as disclosed in EP 0 895 880 A2, for example. According to the example, a frequency shift is given for each wheel fFL, fFR, fRL, fRR (FR: front right, RR: rear right, FL: front left, RL: rear left).
The spread of the temperature Ttire is evaluated when the correction factor 2 is learnt. The correction factor 2 will not be accepted until the spread of the learnt temperature/frequency ensemble with regard to the temperature Ttire (e.g. lowest temperature to highest temperature and a sufficient number of pairs of values above this range) is of sufficient size.
The temperature model 1 uses the following pieces of information, for example, for the calculation of the tire temperature Ttire:
These pieces of information are combined by means of a temperature model 1 which enters the heat flow {dot over (Q)} through flexing energy {dot over (Q)}Walk, convection {dot over (Q)}Convection and radiant heat {dot over (Q)}Radiation into the balance sheet in a first embodiment and calculates a tire temperature therefrom. In another term {dot over (Q)}VehicleCondition for ambient conditions, influences of the vehicle such as brake temperature and engine temperature are taken into consideration.
Possible equations for calculation are:
{dot over (Q)}
Radiation
=ε·σ·A·(Toutside4−Ttire4)=αs(Toutside4−Ttire4)
{dot over (Q)}
Convection=αk·√{square root over (v)}·(Toutside−Ttire)
{dot over (Q)}
Walk
=f·m·g·v=f·F
z
·v
{dot over (Q)}
VehicleCondition
=f(TBrake,TEngine, . . . )
with
ε: emissivity,
σ: Stefan-Boltzmann constant,
A: radiating surface of the tire,
αS: proportionality constant of the radiant heat,
αk: proportionality constant of the convection,
f: proportionality constant of the rolling resistance,
Fz: wheel load,
v: speed,
Toutside: outside temperature,
Ttire: tire temperature, and
f (TBrake, TEngine, . . . ): function of the brake temperature TBrake, the engine temperature TEngine and further quantities.
The tire temperature Ttire can be calculated by integration of the changes of the quantity of heat according to:
with ctire: heat capacity of the tire, and Tstart: start value.
In an especially simple embodiment, the radiation component {dot over (Q)}Radiation is ignored. A minimum speed v in the capacity of an input for the convection equation is assumed as a compensation for the hence missing temperature reduction.
Plausibilisation values from the immobilization time must be taken into account to determine a start value Tstart.
Number | Date | Country | Kind |
---|---|---|---|
10 2005 054 556.4 | Nov 2005 | DE | national |
10 2006 053 825.0 | Nov 2006 | DE | national |
Filing Document | Filing Date | Country | Kind | 371c Date |
---|---|---|---|---|
PCT/EP2006/068442 | 11/14/2006 | WO | 00 | 5/14/2008 |