DETERMINATION OF RUNNING RESISTANCE FOR A VEHICLE

Abstract
A method and a system for determining a running resistance Fres for a vehicle. A model-based running resistance Fres,mod is estimated. Thereafter an energy change difference ΔWdiff between a model-based estimated energy change ΔWpred and an actual energy change ΔWreal is determined for the vehicle from a starting point to an end point of a distance S which is travelled by the vehicle. A braking force Funknown which is unknown to the model and which acts upon the vehicle over the distance S is also determined on the basis of the energy change difference ΔWdiff. Thereafter the running resistance Fres is determined to an adjusted value of the model-based estimate of the running resistance Fres,mod, the adjustment being based on the braking force Funknown which is unknown to the model.
Description
TECHNICAL FIELD

The present invention relates to a method for determining a running resistance Fres for a vehicle according to the preamble of claim 1, a system for determining a running resistance Fres for a vehicle according to the preamble of claim 19, and a vehicle according to the preamble of claim 20. The present invention relates also to a computer programme and a computer programme product which implement the method according to the invention.


BACKGROUND

A vehicle is acted upon by a variety of forces schematically illustrated in FIG. 1. An equation describing these forces may be written as






m{dot over (v)}=F
drive
−F
res
−mg sin α=Fdrive−Fdrivelinelosses−Froll−Fair−mg sin α  (eq. 1)


in which

    • m{dot over (v)} is the vehicle's weight m multiplied by the vehicle's acceleration {dot over (v)} to represent the total amount of forces acting upon the vehicle,
    • Fdrive is the driving force propelling the vehicle, provided mainly by the engine system,
    • Fres=Fdrivelinelosses+Froll+Fair is the running resistance for the vehicle,
    • Fdrivelinelosses is power losses in the power train, e.g. losses in the clutch, transmission and other components of the power train, and the engine system's drag losses depending on the engine system's drag torque,
    • Froll is the rolling resistance for the vehicle,
    • Fair is the air resistance for the vehicle, and
    • mg sin α is the force of gravity acting upon the vehicle at a road gradient α.


The running resistance Fres is employed in many applications in a vehicle. For example, decisions by cruise controls and automatic gearchange systems are based inter alia on the magnitude of the running resistance. It is therefore very important to be able to estimate the running resistance correctly and efficiently.


Today's economical cruise controls take account inter alia of running resistance Fres. Traditional cruise controls maintain a constant reference speed vref which corresponds to the speed vset chosen by the driver. The value of the reference speed vref is only altered when the driver adjusts the set speed vset while driving. Certain economical cruise controls, e.g. Ecocruise cruise controls, have knowledge of the historical running resistance Fres,hist and try also to estimate a current running resistance Fres,pres.


An experienced driver of a vehicle without cruise control can reduce fuel consumption by adapting his/her driving to the characteristics of the road ahead so that unnecessary braking and/or fuel-consuming acceleration can be avoided. A further development of the aforesaid economical cruise controls tries to mimic the experienced driver's adaptive driving on the basis of knowledge of the road ahead so that fuel consumption can be kept as low as possible, since this very greatly affects profitability for an owner of the vehicle, e.g. a haulage company or the like.


An example of such a further development of an economical cruise control is a “look ahead” cruise control (LACC), i.e. an intelligent cruise control which uses knowledge of road sections ahead, i.e. knowledge of the characteristics of the road ahead, to determine the configuration of the reference speed vref. Here the reference speed vref is therefore allowed, within a certain speed range, to differ from the set speed vset chosen by the driver, in order to run the vehicle in a way which saves more fuel.


Knowledge of the road section ahead may for example comprise prevailing topography, road curvature and state of the road on the section ahead. This knowledge may for example be obtained from location information, e.g. GPS (global positioning system) information, map data and/or topographical map data, and weather reports. With an intelligent cruise control which takes account of the topography ahead, i.e. a look-ahead cruise control, it is therefore possible to optimise the vehicle's reference speed vref for different kinds of road, performance and train weight in order to achieve fuel saving.


An economical cruise control can, inter alia on the basis of the forces which act upon the vehicle, i.e. on the basis of the force equation (eq. 1), predict for example the vehicle's speed along a horizon of any suitable length, e.g. 1-2 km. The vehicle's future speed along the horizon may be predicted in various ways, e.g. by assuming that it will run with traditional cruise control with a reference speed vref which is the same as the set speed vset, or by assuming that the reference speed vref is allowed to vary relative to the set speed vset.


A look-ahead cruise control (LACC) does for example allow the reference speed vref to be raised, before an upgrade, to above the set speed vset, since the vehicle will presumably lose speed on the upgrade owing to high train weight relative to engine performance. Similarly, the LACC allows the reference speed vref to drop to below the set speed vset before a downgrade on which the vehicle will presumably be accelerated by its train weight. The concept here is that it is better from a fuel economy perspective to take advantage of the vehicle's acceleration by its own weight downhill than to initially accelerate before the downgrade and then brake on the downgrade. The LACC can thus reduce fuel consumption without greatly affecting journey time. Being able to determine the reference speed vref so that these fuel savings can be achieved depends on good knowledge of the vehicle's force equation (eq. 1), i.e. good knowledge of the forces which act upon the vehicle. The running resistance Fres is one of these forces.


There are also cruise controls which use a running resistance Fres as a basis for deciding how the vehicle's speed should vary. This means that such cruise controls can allow the reference speed vref to deviate from the set speed vset on the basis of at least one characteristic of the running resistance, e.g. its magnitude over time.


According to prior art described in DE102006029366, the running resistance Fres is estimated continually on the basis of the vehicle's acceleration. Such estimation may involve problems, as described in more detail below.


BRIEF DESCRIPTION OF THE INVENTION

It is important for systems which employ the running resistance Fres in their calculations to have available a correct value for the running resistance Fres. If these systems have access to only unreliable or incorrect values for the running resistance Fres, this may lead to dangerously and/or uneconomically wrong decisions due to these deficient or unavailable values for the running resistance Fres.


As mentioned above, certain prior art solutions estimate the running resistance Fres continuously on the basis of the vehicle's acceleration. Such estimation needs to be based on knowledge of road gradient α and vehicle weight m. But such knowledge is most commonly itself based on estimates which inevitably entail further uncertainties. The prior art methods thus often result in an estimate of the running resistance Fres which is impaired by errors, potentially leading to wrong decisions by systems which employ this incorrect estimate.


An object of the present invention is to propose a more efficient and more correct determination of the running resistance Fres which reduces the risk of wrong decisions in a vehicle.


This object is achieved by the aforesaid method for determining a running resistance Fres for a vehicle, according to the characterising part of claim 1. It is also achieved by the aforesaid system for determining a running resistance Fres for a vehicle according to the characterising part of claim 19, by the aforesaid vehicle according to the characterising part of claim 20, and by the aforesaid computer programme and computer programme product.


The present invention makes it possible for simple and computationally efficient models for the vehicle's driving force Fdrive, rolling resistance Froll and air resistance Fair for the vehicle to be employed in determining the running resistance Fres. These simple models also require only a limited amount of storage space to be able to conduct the modelling as compared with more complicated models.


The present invention determines the running resistance on the basis of a change in the vehicle's energy ΔWdiff over a distance S. The result is an average value, i.e. an extracted filtered value, for the difference in the change in energy ΔWdiff. This average value may also be regarded as a physically averaged value when the effect of the forces over a distance/time is employed instead of momentary forces acting upon the vehicle, thus employing an averaged value for the effect of the forces. In other words, the average value of the energy change difference ΔWdiff is based on a non-momentary value for the forces. Basing the calculations on an energy change over a distance instead of on the basis, as in prior art methods, of momentary values of, for example, an acceleration signal, means that fewer calculations need be done and that the values arrived at are of high quality since they take account of variations over the whole distance S. This average value will for example be less sensitive to gusty winds.


Various embodiments of the present invention make advantageous choices of when and/or where to determine the vehicle's running resistance. These choices of time and/or place for such determination result in fewer and simpler calculations for determining the running resistance.


According to an embodiment of the invention, the determination of the energy change difference ΔWdiff may with advantage be done when the running resistance Fres is considerably greater than the driving force e.g. when Fdrive is substantially zero (0) N. The determination thus takes place here when the engine is dragged and is contributing substantially no propulsive force. The calculations are thus simplified.


According to an embodiment of the invention, the determination of the energy change difference ΔWdiff may with advantage be done when the running resistance Fres dominates the force equation, i.e. when Fres constitutes a large proportion of the forces in the force equation (eq. 1) for the vehicle. The calculations are thus likewise simplified. If for example the driving force Fdrive is zero (0) N and the respective road segment is level, the running resistance Fres accounts for 100% of the forces in the righthand member of the force equation (eq. 1).


According to an embodiment of the present invention, the determination of the energy change difference ΔWdiff may with advantage be done when the vehicle effects a speed change, e.g. a retardation. This reduces the impact of any uncertainty about whether an estimate of the vehicle's weight m corresponds to its actual weight.


According to an embodiment of the present invention, the determination of the energy change difference ΔWdiff should be done when the road section covered by the distance S is substantially level at least in places, i.e. when the section S comprises one or more substantially level portions. This likewise reduces also the influence of the vehicle's weight m on the determination of the running resistance Fres.


An example of an occasion which according to the present invention is very appropriate for determining the running resistance Fres is just before a downgrade. The road gradient α is generally slight at the approach to a downgrade. Economical cruise controls which take account of road sections ahead usually effect also a retardation just before a downgrade. On such occasions there are therefore no unknown driving forces acting upon the vehicle and the impact of uncertainty about the vehicle's weight m is also minimised. The result may be a very reliable and simple estimate of the running resistance Fres.


Access to the running resistance determined correctly by the present invention makes it possible for systems which employ the running resistance in their calculations, e.g. economical cruise controls which take account of road segments ahead, to make well-founded and correct decisions. This means that the vehicle's total fuel consumption can be reduced if this is prioritised. Similarly it is also possible to achieve, for example, a more powerful vehicle if this is prioritised, as in the “power mode” application.


It is then also possible to utilise the whole speed range which the cruise control is allowed to use, thereby also reducing fuel consumption. This is because there is greater potential for controlling the vehicle so that it reaches the low initial speed at which it should be just before, rather than long before, it begins to be accelerated by gravity. This is viewed as positive by drivers, thereby boosting acceptance of the cruise control's function and hence also increasing the use of the cruise control. This makes it possible, for example, for total fuel consumption over time to be reduced if this is prioritised.


Adaptation, i.e. determination, of the running resistance Fres is relatively quick by the present invention. The result after even only a small number of determinations before, for example, relatively steep downgrades, is a very reliable value for the running resistance Fres.


In this specification the invention is primarily exemplified for use in a cruise control system, e.g. a look-ahead cruise control (LACC), i.e. an intelligent cruise control which can use knowledge of the nature of the road ahead to control the reference speed vref. The invention might however be implemented in substantially all systems which employ the running resistance Fres in their calculations. One skilled in the art will therefore appreciate that the value determined for the running resistance Fres is usable not only in cruise control but also in substantially all applications where Fres is relevant.





BRIEF LIST OF DRAWINGS

The invention is explained in more detail below with reference to the attached drawings, in which the same reference notations are used for similar items, and in which



FIG. 1 depicts forces which act upon a vehicle,



FIG. 2 is a flowchart for the method according to the invention,



FIG. 3 depicts speed curves for a vehicle on a downgrade,



FIG. 4 depicts various examples of extents for the distance S, and



FIG. 5 depicts a control unit which works according to the invention.





DESCRIPTION OF PREFERRED EMBODIMENTS

The present invention results in very correct estimation of the running resistance for a vehicle. FIG. 2 is a flowchart for the method for determining the running resistance according to the invention. As a first step 201, the method according to the invention estimates a model-based running resistance Fres,mod. Using the invention makes accurate determinations of the running resistance possible even when using relatively simple models in this model-based determination of the running resistance. It is therefore possible for example for models which are simple and computationally not complex to be used for model-based determinations of, for example, the vehicle's driving force Fdrive, rolling resistance Froll and air resistance Fair, as described in more detail below.


As a second step 202, the method according to the present invention determines an energy change difference ΔWdiff for the vehicle between an estimated energy change ΔWpred and an actual energy change ΔWreal.





ΔWdiff=ΔWpred−ΔWreal  (eq. 2)


(One skilled in the art will appreciate that equation 2 may also be expressed as ΔWdiff=ΔWreal−ΔWpred)


This energy change difference ΔWdiff is determined for a distance S travelled by the vehicle, which distance has a starting point and an end point which are different. What is therefore analysed here is how well the estimated energy change ΔWpred and the actual energy change ΔWreal correspond. As the model on which the estimated energy change ΔWpred is based rarely corresponds exactly to reality, there is most commonly an energy change difference ΔWdiff, which is therefore here determined.


As a third step 203, the method according to the invention determines a braking force Funknown which is unknown to the model and which acts upon the vehicle over the distance S. The estimated energy change ΔWpred determined on the basis of the model takes no account of this unknown force Funknown, since it has no knowledge of it. This force Funknown is therefore one of several possible reasons for a difference ΔWdiff between the estimated energy change ΔWpred and the actual energy difference ΔWreal. According to the invention, the energy change difference ΔWdiff determined can therefore be used to determine this braking force Funknown which is unknown to the model.


The braking force Funknown unknown to the model may for example be determined by dividing the energy change difference ΔWdiff by the respective distance S over which the vehicle loses this energy, i.e.







F
unknown

=



Δ






W
diff


S

.





This determination is based on the integral equation







Δ






W
diff


=



0
S




F
unknown








s







in which the unknown braking force Funknown is integrated with respect to the vehicle's location, thus arriving at the work performed by the unknown braking force Funknown over the distance S. The integral equation results in the simple equation ΔWdiff=Funknown*S when all the braking forces are acting in an opposite direction to the vehicle's direction of travel, in which case the simple equation







F
unknown

=


Δ






W
diff


S





produces a reliable value for the unknown braking force.


As a fourth step 204 of the present invention, the model-based estimate of the running resistance Fres,mod is adjusted on the basis of the braking force Funknown which is unknown to the model. The result is a substantially correct value for the running resistance Fres. The running resistance Fres is thus here determined by the model-based estimate of the running resistance Fres,mod being adapted with respect to the force Funknown unknown to the model, making it possible to arrive at a more correct value for the running resistance Fres.


The present invention can be used to make a very good estimate of the running resistance Fres on the basis of models which are simple, do not require particularly large amounts of memory and are computationally efficient, e.g. for the vehicle's driving force Fdrive, rolling resistance Froll and air resistance Fair, and on the basis of the energy change difference ΔWdiff. The models rarely correspond fully to reality. It may for example be difficult for them to predict how much wind, and from what direction, the vehicle will be affected by on a certain road segment at a certain time, how the state of the road varies over time and along the segment, or whether there is a load on the power train. Loads on the power train comprise here loading by one or more external systems, causing part of the power from the engine system to be consumed by these external systems. An example of such an external system is a cooling system for a refrigerated vehicle. The present invention makes it easy to adapt the aforesaid relatively simple models to the more complicated reality. Where/how the resistance occurs when the invention is used is also insignificant. For the present invention it therefore makes no difference whether the running resistance is for example created by the state of the road or by external systems.


The running resistance is also determined on the basis of an energy change ΔWdiff for the vehicle from a starting point to an end point of a distance S, resulting in a value of high quality for the energy change, since it is not a momentary value. The value for the energy change ΔWdiff which is used by the present invention takes instead the form of an average value for the distance S, or a filtered value of the energy change difference ΔWdiff, which is based on a physical averaging of the forces which act upon the vehicle. According to an embodiment of the present invention, the distance S has a length L which exceeds a predetermined length of any suitable magnitude.


As mentioned above, prior art methods have based running resistance estimates on continuous measurements of the vehicle's acceleration, thus basing many calculations on acceleration signals whose magnitude varies over time because of the noisy characteristics of the acceleration signal. Thus many calculations are here based on a noisy acceleration signal, resulting in estimates of low quality. In contrast, the present invention does fewer calculations, but of higher quality, which are based on the energy change ΔWdiff over a distance S.


The energy change difference ΔWdiff arrived at according to the method comprises a kinetic energy change difference ΔWdiff,k and a potential energy change difference ΔWdiff,p.


According to an embodiment of the present invention, the kinetic energy change difference ΔWdiff,k is a difference between a model-based estimated/predicted kinetic energy change ΔWk,pred and an actual kinetic energy change ΔWk,real. The model-based estimated kinetic energy change ΔWk,pred may here be based on a prediction of a speed of the vehicle. The actual kinetic energy change ΔWk,real is based on an actual speed of the vehicle which can be measured when it is in motion, e.g. on the basis of the rotation speed of the propeller shaft, the gear ratio to the driving axle and the radius of the wheels. For vehicles equipped with an economical cruise control system as described above, vehicle speeds are predicted by the cruise control system along a horizon of any suitable length, since predicted speeds are used by the cruise control. Predicted speeds are therefore available and may be used in determining the running resistance according to this embodiment. A correct value for the running resistance is thus arrived at in a computationally efficient way.


The potential energy change difference ΔWdiff,p is a difference between an estimated potential energy change ΔWp,pred and an actual potential energy change ΔWp,real for the vehicle over the distance S. According to an embodiment of the invention, the energy change difference ΔWdiff is determined (according to equation 2 above) when this potential energy change difference ΔWdiff,p is substantially zero. This is possible if there is good knowledge of the topography, e.g. of the road gradient α over the distance S, which may be used in said determination of the energy difference ΔWdiff. Other methods may be used for determining when the potential energy change difference ΔWdiff,p is substantially zero, e.g. methods based on measurement of altitude change over the distance S, which may for example involve air pressure measurements or GPS technology. When the estimated potential energy change ΔWp,pred and the actual potential energy change ΔWp,real correspond well in this way, if there is for example good topographical knowledge (as described above), the energy change difference ΔWdiff arrived at comprises substantially a kinetic energy change difference ΔWdiff,k, thereby simplifying the calculations of the running resistance. The good knowledge of the road gradient α is thus used in this embodiment of the invention to reduce the uncertainty about and calculations relating to the potential energy when determining the running resistance.


An embodiment of the present invention makes an intelligent and advantageous choice of a suitable occasion for determining the running resistance. By suitable choice of when and/or where to determine the running resistance it is possible to minimise the uncertainty pertaining to parameters which affect the vehicle's energy balance. Intelligent choice of time and/or place for the determination also results in simpler calculations in the actual process of determining the running resistance.


According to an embodiment of the invention, the determination of the energy change difference ΔWdiff takes place at a time when the running resistance Fres for the vehicle is considerably greater than the driving force Fdrive which the engine system imparts to the vehicle. At such times any influence of Fdrive may be disregarded, considerably simplifying the calculations. According to an embodiment, the determination of the running resistance takes place when the driving force Fdrive is substantially zero (0) N, in which case Fdrive may of course be disregarded. According to an embodiment, Fdrive is here regarded as substantially zero (0) N if it is less than five (5) N. As indicated above, the engine's drag losses form part of the power train's power losses Fdrivelinelosses.


According to an embodiment of the invention, the determination of the energy change difference ΔWdiff takes place at a time when the running resistance Fres dominates the vehicle's force equation (eq. 1). According to the invention, the running resistance Fres is regarded as dominating the force equation when it accounts for more than half of the forces in the righthand member of the equation.


The calculations are thus further simplified.


This may be achieved by determining the energy change difference ΔWdiff when the vehicle effects a slight speed change, e.g. a retardation. According to an embodiment, the speed change is regarded as slight if it is not such that a gear change is required or will be effected, since for example a downward gear change affects power train losses Fdrivelinelosses. According to an embodiment, the speed change is regarded as slight if the rolling resistance Froll and/or the air resistance Fair are substantially constant. Determination at the time of the slight speed change, e.g. at the time of the retardation, reduces the impact of any uncertainty about the vehicle's weight m, since the running resistance Fres is large relative to the total force m{dot over (v)} acting upon the vehicle, thereby simplifying the calculations. According to an embodiment, the speed change is regarded as slight if any uncertainty caused by it about the weight m will not result in more than 10% of uncertainty about the running resistance Fres. In other words, determining the energy change difference ΔWdiff takes place when the vehicle effects such a slight speed change that the uncertainty about the running resistance Fres will be not more than 10%.



FIG. 3 depicts schematically an example of the possible pattern of a retardation. It shows two curves, viz. a broken curve representing a predicted speed vpred and a continuous curve representing an actual speed vpred, for a vehicle approaching a downgrade. Initially both vpred and vreal are substantially constant over a period S0-S1. At S1 the torque provided by the vehicle's engine system begins to ramp downwards, whereupon both vpred and vreal decrease. This may for example occur just before a downgrade if the vehicle has an economical cruise control which takes account of topography ahead, e.g. a look-ahead cruise control. The cruise control here therefore demands less engine torque just before the downgrade, since it knows that the vehicle's own weight will cause it to accelerate on the downgrade.


An economical cruise control which takes account of topography ahead predicts the speed vpred for a road segment ahead. This prediction vpred is exemplified by the broken line in FIG. 3. When the cruise control predicts the speed, it may also provide this predicted speed vpred to the system which determines the running resistance Fres. It is of computational advantage to be able to reuse predictions already made by on-board systems when the running resistance Fres is to be determined.


Just after the retardation has begun at S1, i.e. just after the predicted speed vpred and actual speed vreal have begun at S1 to decrease from their initially constant values, the engine system will not contribute any driving torque. In other words, the driving force Fdrive here becomes substantially zero, Fdrive=0, further simplifying the force equation (eq. 1). Using this embodiment thus results in a simplified calculation of the running resistance Fres in that an uncertainty factor is eliminated. This embodiment of the invention thus achieves with fewer calculations a more accurate determination of the running resistance Fres.


As described above, the energy change difference ΔWdiff comprises a kinetic energy change difference ΔWdiff,k and a potential energy change difference ΔWdiff,p, the potential energy change difference ΔWdiff,p in this embodiment being negligible relative to the kinetic energy change difference ΔWdiff,k. The kinetic energy change difference ΔWdiff,k is a difference between a model-based estimated kinetic energy change ΔWk,pred and an actual kinetic energy change ΔWk,real, the model-based estimated change being based on the predicted speed vpred (broken line in FIG. 3) and the actual change being based on the actual speed vreal (continuous line in FIG. 3). As depicted in FIG. 3, vpred and vreal differ, so there is an energy change difference ΔWdiff. As this difference takes the form of the kinetic energy change difference ΔWdiff,k it may be found, as described in more detail below, that the deviation between the predicted speed vpred and the actual speed vreal depends substantially entirely on the running resistance Fres, i.e. on the rolling resistance Froll, the air resistance Fair and power train losses Fdrivelinelosses.


As illustrated in FIG. 3, the predicted speed vpred and the actual speed vreal reach at S2 their respective minima vpred,min and vreal,min which differ in magnitude, before rising again after S2. The vehicle therefore first retards before the downgrade S1-S2 when the cruise control decreases the demand for engine torque, followed by accelerating downhill after S2.


According to an embodiment of the invention, the determination of the energy change difference ΔWdiff takes place at a time when the road section covered by the distance S over which the energy change difference is analysed is substantially level at least in places, i.e. when it comprises one or more substantially level portions. When the road is level, i.e. road gradient zero, α=0, the term for gravity in the force equation (eq. 1) is also zero, mg sin α=0. The influence of the vehicle's weight m on the determination of the running resistance Fres is thus also reduced. This is highly advantageous, since there is rarely good knowledge of the vehicle's weight m. The weight of for example a truck may vary greatly depending on whether it is laden or not, and also on the nature of its cargo.


An occasion when the road gradient α is generally slight is just before a downgrade. Moreover it is by definition zero at the approach to the downgrade. This embodiment of the invention may therefore be employed with advantage at the approaches to downgrades.


According to an embodiment of the invention, the road gradient α is regarded as slight if it is less than or equal to one percent, i.e. 1%≦α≦1%. A stretch of road is regarded as substantially level if its gradient α is slight.


As mentioned above, vehicles with certain economical cruise controls usually also effect a retardation just before a downgrade. At the approach to a downgrade, the force equation (eq. 1) may therefore be considerably simplified in that both the driving force Fdrive and the force of gravity in the equation are zero, Fdrive=0 and mg sin α=0. This is therefore a suitable occasion for determining the running resistance Fres according to the present invention, since any uncertainty about said vehicle's weight m and the driving force Fdrive will have little influence. In other words, according an embodiment the distance S may with advantage be relocated to a road segment after S2 where the vehicle is retarded with substantially no driving engine torque and the gradient α is slight. Over such a distance S, the air resistance Fair and the rolling resistance Froll which form part of the running resistance Fres have a dominant effect on the vehicle's speed, considerably simplifying the calculations.


According to an embodiment of the present invention, the distance S chosen is such that it comprises the point S2 at which the vehicle has a local speed minimum. Thus the distance S should here comprise minima for the respective predicted and actual speeds vpred,min and vreal,min in FIG. 3.


According to an embodiment, this local speed minimum marks the end point of the distance S. This embodiment affords the advantage that local speed minima for which values already determined are available on board, since they are used by other systems, e.g. cruise control systems. This means that the distance S may here begin just before a downgrade, when the retardation has commenced and the driving force Fdrive is substantially zero N, and end at a speed minimum.



FIG. 4 depicts various examples Sa, Sb, Sc of extents for the distance S, which extents may be used according to various embodiments of the invention. For the extent Sa the distance S has its starting point just after the predicted speed vpred and actual speed vreal have begun to drop at S1, and its end point before S2, where the respective predicted and actual speeds vpred,min and vreal,min have their minima.


For the extent Sb the distance S has its starting point just after the predicted speed vpred and the actual speed vreal have begun to drop at S1, and its end point at S2, i.e. at the respective minima of the predicted speed vpred,min and the actual speed vreal,min. The values for the minima of vpred,min and vreal,min are available through having already been determined by the cruise control, resulting in a computationally very efficient way of determining the running resistance.


According to an embodiment of the present invention, the distance S is set as long as possible, subject to being able to make a reliable determination of the running resistance Fres during it. This is illustrated by the extent S, in FIG. 4.


Reliable determination of the running resistance Fres is not possible if a gear change takes place, e.g. during retardation, or if a retardation is discontinued, e.g. by a driver or a cruise control. Nor will determination of the running resistance Fres be reliable if the predicted speed vpred and the actual speed vreal differ considerably, which may for example indicate that the wind direction has changed. The extent chosen for the distance S according to this embodiment is therefore long enough to allow good physical averaging of the forces which act upon the vehicle, but short enough to avoid events which would render the estimation of the running resistance Fres unreliable. According to an embodiment, the predicted speed vpred and the actual speed vreal are regarded as differing considerably if the deviation is more than 4 km/h.


The distance S chosen is therefore such that its end point is relatively near, but does not comprise the aforesaid events which would render the determination unreliable. In practice this is achieved by values being monitored until one of the aforesaid events occurs and by only values before it being then employed in the determination. In this way the distance S chosen will be as long as possible.


In the case of the extent S1 for the distance S in FIG. 4, an event which renders estimating the running resistance Fres unreliable occurs just before the respective minima of the predicted speed vpred,min and the actual speed vreal,min, so the extent S1 is relatively short.


Choosing suitable lengths for the distance S according to the foregoing embodiments results in maximum possible reliability of estimation of the running resistance Fres while at the same time minimising the calculations.


According to an embodiment of the invention, the adaptation of the running resistance Fres is limited/saturated at a predetermined magnitude Y N. This is to prevent for example any error in the weight estimation being incorrectly interpreted as an error in the running resistance estimation. If the weight is estimated incorrectly, the adaptation of the running resistance will also be incorrect. As the adaptation of the running resistance Fres according to this embodiment is limited to a predetermined magnitude Y N, the influence of the incorrectly estimated weight is minimised. Y has here any suitable value.


According to an embodiment of the invention, the adaptation begins again if the vehicle changes roads. Road changes may for example be identified on the basis of road-related GPS information, e.g. on the basis of road number in the case of a road on which a vehicle is located by means of the GPS system. Here the adaptation is therefore zeroed when the vehicle changes road. This means that separate values for the running resistance are arrived at for different roads, which is advantageous in that different roads often have different characteristics. They may for example differ in asphalt quality and/or extent (which may for example affect the vehicle's wind resistance). Thus according to this embodiment a first value for the running resistance would be obtained for a first road with asphalt which is easy to roll on and the vehicle has a tailwind, and a second value for a second road then joined by the vehicle on which the asphalt is hard to roll on and the vehicle has a headwind. It is advantageous to obtain separate and correct values for each road.


According to an embodiment of the present invention, an adjustment parameter kadj is determined on the basis of the braking force Funknown which is unknown to the model. This adjustment parameter kadj is used when determining the running resistance Fres. It may be regarded as an addition to the running resistance which arises from this force Funknown unknown to the model. According to an embodiment, the adjustment parameter kadj is constant over a period of time or for a distance, e.g. along a road. According to an embodiment, it corresponds to the braking force Funknown unknown to the model, i.e. kadj=Funknown.


In more detail, the adjustment parameter kadj may be used to adjust the model-based estimated running resistance Fres,mod. According to an embodiment, it is used as an additive parameter to the other terms of the force equation, i.e. Fres,mod=Fres+kadj. The force equation (eq. 1) then assumes the form






m{dot over (v)}=F
drive
−F
res
−k
adj
−mg sin α  (eq. 3)


According to another embodiment, the adjustment parameter kadj is used as a multiplicative parameter which is multiplied by terms for running resistance Fres in the force equation, i.e. fres,mod=Fres*kadj. It corresponds here to a dimensionless scaling constant kscale, which has a value based on a ratio between an actual value of the running resistance Fres,real and the model-based estimate of the running resistance Fres,mod, i.e.







k
adj

=


k
scale

=



F

res
,
real



F

res
,
mod



.






The force equation (eq. 1) then assumes the form






m{dot over (v)}=F
drive
−k
adj
*F
res
−mg sin α  (eq. 4)


Using the adjustment parameter kadj makes a computationally efficient adjustment of simple models possible so that they become very close to reality.


The present invention relates also to a system for determining a running resistance Fres for a vehicle. The system comprises an estimation unit, a difference unit, a force unit and an adjustment unit. The estimation unit is adapted to estimating a model-based running resistance Fres,mod as described above in relation to the method. The difference unit is adapted to determining the energy change difference ΔWdiff described above between a model-based estimated energy change ΔWpred and an actual energy change ΔWreal, for the vehicle from a starting point to an end point of a distance S which is travelled by the vehicle.


The force unit is adapted to determining, as described above, on the basis of the energy change difference ΔWdiff a braking force Funknown which is unknown to the model and which acts upon the vehicle over the distance S. The adjustment unit is adapted to determining the running resistance Fres to an adjusted value of the estimate of the model-based running resistance Fres,mod. As described above, the adjustment is based here on the force Funknown which is unknown to the model.


One skilled in the art will appreciate that a method for determining the running resistance Fres according to the present invention may also be implemented in a computer programme which, when executed in a computer, causes the computer to apply the method. The computer programme usually takes the form of a computer programme product 503 (in FIG. 5) stored on a computer-readable medium which contains the computer programme. Said computer-readable medium comprises a suitable memory, e.g. ROM (read-only memory), PROM (programmable read-only memory), EPROM (erasable PROM), flash memory, EEPROM (electrically erasable PROM), a hard disc unit, etc.



FIG. 5 depicts schematically a control unit 500 comprising a calculation unit 501 which may take the form of substantially any suitable type of processor or microcomputer, e.g. a circuit for digital signal processing (digital signal processor, DSP), or a circuit with a predetermined specific function (application specific integrated circuit, ASIC). The calculation unit 501 is connected to a memory unit 502 which is situated in the control unit 500 and which provides the calculation unit with, for example, the stored programme code and/or stored data which the calculation unit needs to enable it to do calculations. The calculation unit 501 is also adapted to storing partial or final results of calculations in the memory unit 502.


The control unit 500 is further provided with respective devices 511, 512, 513, 514 for receiving and sending input and output signals. These input and output signals may comprise waveforms, pulses or other attributes which the input signal receiving devices 511, 513 can detect as information and which can be converted to signals which the calculation unit 501 can process. These signals are then supplied to the calculation unit. The output signal sending devices 512, 514 are arranged to convert signals received from the calculation unit in order, e.g. by modulating them, to create output signals which can be conveyed to other systems on board the vehicle.


Each of the connections to the respective devices for receiving and sending input and output signals may take the form of one or more from among a cable, a data bus, e.g. a CAN (controller area network) bus, an MOST (media oriented systems transport) bus or some other bus configuration, or a wireless connection.


One skilled in the art will appreciate that the aforesaid computer may take the form of the calculation unit 501 and that the aforesaid memory may take the form of the memory unit 502.


One skilled in the art will also appreciate that the above system may be modified according to the various embodiments of the method according to the invention. The invention relates also to a motor vehicle, e.g. a truck or bus, provided with at least one system for determining the running resistance Fres according to the invention.


The present invention is not restricted to the invention's embodiments described above but relates to and comprises all embodiments within the protective scope of the attached independent claims.

Claims
  • 1. A method for determining a running resistance Fres for a vehicle comprising: estimating a model-based running resistance Fres,mod;determining an energy change difference ΔWdiff between a model-based estimated energy change ΔWpred and an actual energy change ΔWreal, for said vehicle from a starting point to an end point of a distance S which is travelled by said vehicle;based on said energy change difference ΔWdiff, determining a braking force Funknown which is unknown to the model and which acts upon said vehicle over said distance S; anddetermining said running resistance Fres to an adjusted value of said model-based estimate of said running resistance Fres,mod, said adjusted value is based on said braking force Funknown which is unknown to the model.
  • 2. A method according to claim 1, wherein said energy change difference ΔWdiff comprises a kinetic energy change difference ΔWdiff,k between a model-based estimated kinetic energy change ΔWk,pred and an actual kinetic energy change ΔWk,real.
  • 3. A method according to claim 2, further comprising: basing said model-based estimated kinetic energy change ΔWk,pred on a prediction of a speed for said vehicle; andbasing said actual kinetic energy change ΔWk,real on an actual speed of said vehicle.
  • 4. A method according to claim 2, wherein said determination of said energy change difference ΔWdiff takes place when a potential energy change difference ΔWdiff,p between an estimated potential energy change ΔWp,pred and an actual potential energy change ΔWp,real for said vehicle over said distance S is substantially zero.
  • 5. A method according to claim 2, wherein said determination of said energy change difference ΔWdiff takes place when said running resistance Fres for said vehicle is greater than a driving force Fdrive which acts upon said vehicle.
  • 6. A method according to claim 5, wherein said determination takes place when said driving force Fdrive is substantially zero (0) N.
  • 7. A method according to claim 2, wherein said determination of said energy change difference ΔWdiff takes place when said running resistance Fres for said vehicle dominates a force equation for said vehicle.
  • 8. A method according to claim 2, wherein said determination of said energy change difference ΔWdiff takes place when said vehicle effects a speed change in which an impact of any uncertainty about a weight m of said vehicle is slight.
  • 9. A method according to claim 2, wherein said determination of said energy change difference ΔWdiff takes place when a section of road covered by said distance S is substantially level at least in places along said distance S, such that the impact of any uncertainty about a weight m of said vehicle is slight.
  • 10. A method according to claim 1, wherein said distance S comprises a point where said vehicle's speed has a local minimum.
  • 11. A method according to claim 8, wherein a driving force Fdrive for said vehicle at said starting point is substantially zero (0) N.
  • 12. A method according to claim 1, wherein a road gradient α over said distance S is used in said determination of said energy difference ΔWdiff.
  • 13. A method according to claim 1, wherein said distance S has a length L which exceeds a predetermined length, and said energy change difference ΔWdiff takes the form of an average value over said distance S.
  • 14. A method according to claim 1, wherein said end point is before a point where any of the following occurs: gear change;discontinuation of a retardation on the basis of input by a user;discontinuation of a retardation on the basis of intervention by a cruise control; ordetection of a considerable difference between a predicted speed vpred and an actual speed vreal.
  • 15. A method according to claim 1, further comprising determining an adjustment parameter kadj based on said braking force Funknown which is unknown to the model, and using said parameter in said determination of said running resistance Fres.
  • 16. A method according to claim 15, wherein said determining of said running resistance Fres includes using kadj as an adjustment parameter for said model-based estimated running resistance Fres,mod, wherein said parameter is either an additive parameter; ora multiplicative parameter.
  • 17. (canceled)
  • 18. A computer program product comprising a non-transitory computer-readable medium having a computer program comprising program code and which when said code is executed in a computer, causes said computer to apply said method according to claim 1.
  • 19. A system configured for determining a running resistance Fres for a vehicle, said system comprising: an estimation unit configured for estimating a model-based running resistance Fres,mod;a difference unit configured for determining an energy change difference ΔWdiff between a model-based estimated energy change ΔWpred and an actual energy change ΔWreal for said vehicle from a starting point to an end point of a distance S which is travelled by said vehicle;a force unit configured for determining, based on said energy change difference ΔWdiff, a braking force Funknown which is unknown to the model and which acts upon said vehicle over said distance S; andan adjustment unit configured for determining said running resistance Fres to an adjusted value of said model-based estimate of said running resistance Fres,mod and basing said adjustment on said braking force Funknown which is unknown to the model.
  • 20. A vehicle having a system configured for determining a running resistance Fres according to claim 19.
Priority Claims (1)
Number Date Country Kind
1150593-0 Jun 2011 SE national
PCT Information
Filing Document Filing Date Country Kind 371c Date
PCT/SE2012/050652 6/15/2012 WO 00 12/13/2013