BJ1042輕型載貨汽車前懸架設(shè)計(jì)【前雙橫臂獨(dú)立懸架】
BJ1042輕型載貨汽車前懸架設(shè)計(jì)【前雙橫臂獨(dú)立懸架】,前雙橫臂獨(dú)立懸架,BJ1042輕型載貨汽車前懸架設(shè)計(jì)【前雙橫臂獨(dú)立懸架】,bj1042,輕型,載貨,汽車,懸架,設(shè)計(jì),前雙橫臂,獨(dú)立
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Spring into Action.
The recent development of the Lotus active suspension system has proved that car body movements such as pitch and roll can be precisely controlled. Unfortunately it will take some time before we can all take advantage of these developments, and in the meantime we are stuck with the conventional springs and suspension that seems to have changed little since the days of the horse drawn carriage.
Every enthusiast knows that the roll characteristics of a car have considerable influence on its dynamic behaviour as well as the comfort of its occupants. The parameters that control these characteristics are numerous, terms such as roll centre, roll stiffness, roll axis and roll couple are often bandied about but seldom adequately explained. I have often seen, in books and magazine articles, geometric constructions that can be used to determine roll centres and axis for different suspension layouts, but I have never seen an explanation of why these methods actually provide this information. It seems to be taken for granted that the reader will just accept it on face value, or is it because the writer is unsure himself and is just repeating that which he has read elsewhere. Anyway let's break with tradition and see if we can untangle the subject.
Firstly, we must understand the terminology. The roll axis is an imaginary line running through the car from end to end; when the car rolls, whilst cornering on a smooth road, it rotates about this axis. Any part of the vehicle not on this axis bodily moves, either up or down, side to side or both. Fig 1 shows the motion, as well as the longitudinal position of the roll centres, these usually being points on the roll axis in line with the wheels. Note that there's no theoretical reason why the roll centre heights should be at the same level at each end, and indeed they rarely are.
Now before going into the details of determining the roll centre and axis location, it must be understood that these parameters are not fixed in relation to the car's chassis, but move about depending on the deflection of the suspension and therefore vary depending on the roll angle which is influenced by the cornering force. When the car rolls the suspension on one side is compressed and on the other it becomes extended, for the purposes of analysis it matters not whether we consider the wheels as fixed and the body as capable of movement relative to them, or the body as fixed with wheels capable of moving. But as it is easier to visualise the motion with a fixed chassis we will go with that.
Let's now con
sider the case of a double wishbone
suspension system as in Fig 2. If we allow a very small vertical wheel displacement to take place, then the path of this movement (at the wheel end of the wish- bones) is at right angles to the wishbones, therefore the length of the wishbone does not affect the geometry of movement of the upright and wheel (for small displacements). So if the wishbones were extended in length until their inner pivots coincide then the motion of the wheel would be unaffected, but as the two wishbones now pivot around the same axis, we could replace them with a single arm fixed to the wheel axle, thus in effect creating an equivalent swing axle suspension system.
Because this new swing axle is only a figment of our imagination, let's call it a 'virtual swing axle' and its pivot a 'virtual pivot'.
Now, we need to consider the motion of the wheel at the tyre contact patch because this is our only connection with terra-firma, the reference from which we measure the roll. The diagram shows that this motion is at right angles to the line connecting the virtual pivot and the contact patch. Again for small deflections, this motion is unchanged as long as the effective pivot is located anywhere along this line. A mirror image of this applies to the wheel at the other side also. Thus the only common pivot point that satisfies both sides is the one at the junction of these lines, through the contact patches to the respective virtual pivots.
So if there is one pivot point that can relate the motion of both tyre contact patches relative to the chassis, then that same point locates the chassis relative to the wheels. It is the point about which the body will pivot should the suspension on one side be compressed by the same amount as the suspension on the other side be extended, in other words it is the roll centre.
I have emphasised the point about small wheel displacements, this is very important because the roll centre may vary its position enormously throughout the range of normal wheel movement. As the car rolls, its roll centres may change not only in height but also from side to side, as Fig 3, demonstrates.
Even though we have used a double wishbone system to explain the method of determining the roll centre position, it is very easy to apply the method to any other suspension configuration. It is only necessary to determine the directions of movement of the contact patches, and draw lines at right angles to these through the contact patches, the point at which these last two lines cross is the roll centre. Fig 4, shows the method for several different systems.
All of the above makes one big assumption (anyone spot it?) that the effective spring rates at the wheels are equal side to side. But aren't they, I hear you ask. No, not always: what if you have progressive rate springing? The effective spring rate will be increasing on the side that is compressing and will be reducing on the other. To understand the effect that this may have, let's look at the extreme case of a car with a rigid suspension on one side only and with a normal spring on the other. The chassis is thus completely tied to one contact patch and so this is the only point about which it can roll. Thus the roll centre is at ground level directly under the wheel with the infinitely stiff springing. Obviously this situation is unreal but demonstrates how the actual roll centre moves away from the geometrically constructed one, if the springing is not symmetrical.
It is all very well knowing where the roll centres and thus the roll axis are but what use is that knowledge, how can we use it and where should they be anyway? To answer this, we need to look at the superficially obvious question, 'Just what causes roll?'.
As we negotiate a curve the car is subject to centrifugal force, which is equal to the lateral acceleration multiplied by the mass of the machine (for a 1000Kg car cornering at 0.5g. The centrifugal force is 500Kg). This force is distributed throughout the car but for most analysis purposes can be considered to be acting only through the centre of gravity (C of G). Fig 5, shows that unless the C of G is level with the roll axis, a torque or couple (the roll couple) will be created, tending to make the machine roll about the roll axis.
There is another equally valid way of considering the roll mechanism. The centrifugal force acting through the C of G produces a torque about ground level and is resisted by weight transfer to the outside wheels, that is, the outside wheels support a greater proportion of the car's weight and the inside wheels a lesser proportion.
This change of load on each wheel normally causes the suspension to adopt a new position, or to put it another way the car rolls.
It may have occurred to some of you that if the roll axis is made to coincide with the C of G then there will be no roll couple and hence no roll or, to take things a step further, if the roll axis is above the C of G then the roll couple will be in a direction which makes the car lean inward like a motorbike. Indeed it is quite possible to design the suspension layout to achieve these effects. If this is so, why do we need active suspension to do it for us? Well, because if we use the high roll axis necessary, then the suspension layout will cause a jacking up effect under cornering conditions, a phenomenon experienced with some swing axle designs in the past.
One important point to note, one which is often misunderstood, is that regardless of the amount of roll allowed by the suspension design, the actual degree of weight transfer remains unchanged. This is only affected by the track, C of G height and cornering acceleration.
So, as with most design features in anything mechanical, the selection of roll axis position is a compromise: too low and we get excessive roll, too high and other undesirable handling traits surface. In practice, the com- promise varies with different types of car but always such that some roll occurs. Lowering the C of G is another technically possible way of reducing the roll couple, but this can only be done to a certain extent, due to the boring necessity of leaving comfortable space for the occupants.
The roll couple that such compromise leaves must be resisted by the car's springs, which leads us to roll stiffness. This term is defined such that the degree of roll is equal to the roll couple divided by the roll stiffness. Stiff springing obviously reduces roll and hence increases the roll stiffness, but if this is the criterion for selecting spring rates we will usually end up with an uncomfortable ride over normal road irregularities, so the anti-roll bar was developed to ease the situation.
The anti-roll bar is a torsion bar (torsion spring) connecting the suspension systems on each side of the vehicle in such a way as to allow both wheels to respond unhindered to two-wheel bumps, such as a ridge across the road. But if the wheels try to move independently, as with a single-wheel bump, or in opposite directions when the car rolls then the anti-roll bar resists this tendency. Roll is reduced as intended but comfort suffers as the effective spring rate of each wheel is increased in the individual single-wheel bumps, although the combined spring rate of the two wheels is unchanged over joint disturbances.
Again a compromise must be reached between the requirements of minimum roll and good response to road shocks. Roll bars, unlike the springs, are undamped (theoretically damping could be incorporated, although the manufacturers have generally concluded that it is not worthwhile). This is another reason for limiting the influence of the anti-roll bar, as oscillations might occur if the undamped bar is too stiff.
It is well known that the under/over steering characteristics of a car can be substantially modified by tuning the springing and anti-roll bar stiffnesses, altering the roll stiffnesses of each end.
While the vehicle as a whole has a certain roll stiffness, this is made up of the separate roll stiffnesses at the front and back, which may be quite different. For example, let's consider the case of a beam axle pivotted on the chassis at its mid point, and devoid of any form of springing. As unlikely as this layout seems, you may see it fitted to the front of some tractors, because it has good terrain-following properties. Now, because the chassis is completely free to rotate about the pivot point of this beam axle, then no roll stiffness is provided at this end of the machine and so all the stiffness needed must be available from the other end.
This lack of any roll stiffness means that body roll cannot cause any weight transfer to the outside wheel, and hence as the total weight transfer must be the same anyway, the other end must obviously be subjected to proportionally more.
Tyres have the interesting property that although they are capable of supporting higher cornering forces when subject to higher vertical loading, this does not go up in proportion. In other words, the co-efficient of friction is reduced as more weight is placed on them. In practice this means that weight transfer reduces the combined cornering force capable of being developed by the pair of tyres at one end of the car. Now as we have seen, the weight transfer at either end of the vehicle can be controlled to some extent by altering the roll stiffnesses of one or other, or both ends. Therefore, the tyre slip angles needed to produce the required cornering forces can be adjusted by modifications to the wheel springing, thus giving us the means to alter the under/over steering properties.
Dampers, too, have their part to play in the extremely complex interrelations between the various forces acting on the car. During the transitional period between initiating a turn and it becoming fully established, the dampers will affect the dynamic roll stiffnesses. Because the dampers only contribute whilst the suspension is actually moving, however, they have no effect once the car has settled down to a steady state turn.
So now you know why racers spend so much time setting up the suspension rates on their machines, when at first sight it would appear that the suspension is there only to cushion the bumps. Many competition cars have facilities for altering roll bar stiffness whilst on the move, making it quicker to achieve the desired performance but also allowing adjustments during a race as tyres wear and fuel weight reduces.
So how will active suspension improve the situation? The computer program controlling the system could, for example, be set to apportion the front/rear roll stiffness.
Assuming, that the system is set to give zero roll (this is by no means certain to be the aim of future manufacturers) then it is very interesting to follow through the implications for geometric roll centres, etc. Basically if we have no roll then the term roll axis becomes irrelevant, as does the need to have suspension link layouts that try to keep the outside wheels upright under cornering roll rather than under all conditions. Perhaps active suspension means a return to parallel equal length wishbones or perhaps better still, true trailing or leading arm systems. Normally, these designs suffer because of vast changes in roll centre positions, and because the camber angle varies with the roll angle of the body, the wheels always being held parallel to it. Straight line stability would be improved as bump induced wheel deflections would not cause any of the bump steer which comes from changing wheel camber. That's a desirable state of affairs that is hard, if not impossible to achieve with conventional springs and dampers as we have seen.
彈性運(yùn)動(dòng)
近來(lái)蓮花主動(dòng)懸架系統(tǒng)的發(fā)展證明了汽車車身像前傾后仰和反轉(zhuǎn)這樣的運(yùn)動(dòng)時(shí)是可以準(zhǔn)確的控制的。令人遺憾的是在我們能夠利用所有的這些成果之前還將花費(fèi)一些時(shí)間的。與此同時(shí)我們無(wú)法擺脫從四輪馬車時(shí)就有的只是看起來(lái)有些很小的變化的彈簧和懸架。
每一個(gè)愛(ài)好者都知道汽車的側(cè)傾性對(duì)汽車的動(dòng)力性表現(xiàn)和乘坐舒適性有很大影響。這些參數(shù)控制這些特性是很多方面的，例如側(cè)傾中心、側(cè)傾剛度、側(cè)傾軸線和側(cè)傾力矩是經(jīng)常被討論的但是很少給出合適的解釋。我曾經(jīng)經(jīng)常在書中和雜志文章中看到運(yùn)用幾何構(gòu)造學(xué)來(lái)決定對(duì)于不同懸架安排的側(cè)傾中心和側(cè)傾軸線，但是我從來(lái)沒(méi)有看見(jiàn)一種解釋為什么這種方法真正可以提供這些信息。這似乎被認(rèn)為假定讀者只是表面認(rèn)同這種方法，或者是不是因?yàn)樽髡弑救艘膊淮_定，只是重復(fù)他從別處讀來(lái)的。無(wú)論如何讓我們打破傳統(tǒng)來(lái)看看我們是否能解開(kāi)這個(gè)問(wèn)題。
首先我們必需了解一些專用術(shù)語(yǔ)。側(cè)傾軸線是虛構(gòu)的一條從汽車的一端到另一端的直線；當(dāng)汽車側(cè)傾時(shí)，當(dāng)在一段光滑的路面上轉(zhuǎn)彎時(shí)，汽車?yán)@著這條軸線旋轉(zhuǎn)。這條軸線上的汽車任何部分都不移動(dòng)，既不向上也不向下，也不從一邊到另一邊運(yùn)動(dòng)或者兩者都有。圖1展示了這種運(yùn)動(dòng)，同時(shí)也展示了側(cè)傾中心的縱向位置，通常側(cè)傾中心在側(cè)傾軸線與車輪軸線的交點(diǎn)處。注意到?jīng)]有理論原因?yàn)槭裁磦?cè)傾中心的高度在兩頭應(yīng)該在統(tǒng)一水平線上，而且事實(shí)上它們很少在同一水平線上。
現(xiàn)在在進(jìn)入決定側(cè)傾中心和軸線的位置的細(xì)節(jié)之前，必須明白這些參數(shù)對(duì)于汽車底盤并不是固定不變的，而是根據(jù)懸架的傾斜而運(yùn)動(dòng)，因此是根據(jù)由側(cè)向力引起的側(cè)傾角而變化的。當(dāng)汽車旋轉(zhuǎn)時(shí)一側(cè)的懸架壓縮另一側(cè)的懸架伸張，分析它的目的是關(guān)系到我們應(yīng)該認(rèn)為車輪不動(dòng)而車身相對(duì)車輪是可以運(yùn)動(dòng)的，還是應(yīng)該認(rèn)為車身不動(dòng)而車輪可以運(yùn)動(dòng)。但是當(dāng)把固定的底盤想象成運(yùn)動(dòng)的是比較容易的時(shí)候我們就會(huì)這樣去做。
現(xiàn)在讓我們考慮如圖2的雙橫臂懸架系統(tǒng)的情況。如果允許垂直車輪發(fā)生一個(gè)很小的位移，那么這個(gè)運(yùn)動(dòng)的路徑（在橫臂末端的車輪上）相對(duì)于橫臂成直角，因此橫臂的長(zhǎng)度不影響垂直車輪的運(yùn)動(dòng)幾何學(xué)（因?yàn)槲灰坪苄。?。因此如果橫臂延長(zhǎng)至它們的內(nèi)側(cè)軸相交那么車輪的運(yùn)動(dòng)就不會(huì)受影響，但是如果兩個(gè)橫臂繞一個(gè)軸轉(zhuǎn)動(dòng)，我們就可以把它們?cè)O(shè)置成一個(gè)橫臂固定到車輪軸上，因此實(shí)際上等價(jià)于一個(gè)等長(zhǎng)的擺動(dòng)軸的懸架系統(tǒng)。
因?yàn)檫@種新的擺動(dòng)軸只是我們?cè)O(shè)想的虛構(gòu)的，我們叫它虛擬擺動(dòng)軸和它的軸線叫做虛擬擺動(dòng)軸線。
現(xiàn)在我們需要考慮車輪輪胎邊緣處的運(yùn)動(dòng)因?yàn)檫@是我們唯一與泥土相接觸的，作為我們測(cè)量滾動(dòng)的參考。上圖展示了這個(gè)運(yùn)動(dòng)與連接虛擬軸線和接觸邊緣的線成直角。
所以如果有一個(gè)軸線點(diǎn)能夠使兩個(gè)輪胎接地點(diǎn)的運(yùn)動(dòng)相對(duì)于懸架有關(guān)聯(lián)，也就是相對(duì)于車輪在懸架上的點(diǎn)。這一點(diǎn)就是車身繞其旋轉(zhuǎn)的點(diǎn)，懸架的一側(cè)伸張，另一側(cè)壓縮，換句話說(shuō)這就是側(cè)傾中心。
我已經(jīng)強(qiáng)調(diào)國(guó)這一點(diǎn)關(guān)于車輪的小位移，這是非常重要的因?yàn)樵谲囕喺＿\(yùn)動(dòng)時(shí)側(cè)傾中心可能變化很大。當(dāng)車側(cè)傾時(shí)它的側(cè)傾中心不僅可能在垂直方向改變也可以在水平方向改變，參見(jiàn)圖3所示。
雖然我們已經(jīng)用雙橫臂懸架解釋了如何確定側(cè)傾中心的位置，將這種方法運(yùn)用到其它任何懸架結(jié)構(gòu)是很簡(jiǎn)單的。只是需要確定接觸邊緣的運(yùn)動(dòng)方向，通過(guò)接觸邊畫直角線，兩條線的交點(diǎn)就是側(cè)傾中心。圖4展示了這種方法運(yùn)用在一些不同的系統(tǒng)中。
以上的全部做了一個(gè)大膽的假設(shè)（有人能指出來(lái)么？）那就是兩邊車輪的彈性是一樣的。但是它們不一樣么，我聽(tīng)見(jiàn)你問(wèn)了。是的，不總一樣：除非你有非常先進(jìn)的等比彈性材料。實(shí)
際的彈性特性是在被壓縮的一邊增加另一邊減少。為了理解可能導(dǎo)致的后果，讓我們看看極限情況，一邊的懸架是剛性的另一邊有正常彈簧。底盤因此完全和一邊的接觸邊緣相連，這
樣這就是唯一的懸架能夠繞其轉(zhuǎn)動(dòng)的點(diǎn)。因此側(cè)傾中心在極其堅(jiān)硬的剛性車輪的沿地平線的后面。顯然這種情況是假的但是卻論證了如果彈性不對(duì)稱，側(cè)傾中心是如何從原來(lái)的由幾何學(xué)確定的位置移動(dòng)的。
這樣就很好的了解了側(cè)傾中心的位置也就知道了側(cè)傾軸但是這有什么用呢,我們?cè)趺磻?yīng)用它呢和在任何工況下它們的位置應(yīng)該是怎樣的呢？為了回答這個(gè)問(wèn)題，我們需要看看一個(gè)顯而易見(jiàn)的問(wèn)題“到底是什么引起側(cè)傾的呢”？
大家都知道轉(zhuǎn)彎時(shí)汽車受離心力影響，這個(gè)力等價(jià)于隨著質(zhì)量的增加而增加的側(cè)向加速度（1000千克的汽車在0.5g的情況下轉(zhuǎn)彎。離心力時(shí)500千克）。這個(gè)力被分解到汽車的每一個(gè)部分但是為了分析的目的可以認(rèn)為這個(gè)力只作用在重心上。如圖5所示，除非重心與側(cè)傾軸平行，力矩或者轉(zhuǎn)矩（側(cè)傾轉(zhuǎn)矩）就會(huì)產(chǎn)生，就產(chǎn)生汽車?yán)@側(cè)傾軸轉(zhuǎn)動(dòng)的傾向。
由另一個(gè)等價(jià)的令人信服的方法可以討論這個(gè)側(cè)傾的機(jī)器。離心力作用通過(guò)重心產(chǎn)生一個(gè)關(guān)于地平線的力矩和轉(zhuǎn)移到外側(cè)車輪的重力的抵抗，這樣外側(cè)車輪支持汽車較大的重量而內(nèi)側(cè)車輪支持較小的重量。
每個(gè)車輪的這種載荷的變化引起懸架需要適應(yīng)一種新的位置，或者使汽車進(jìn)入另一種側(cè)傾方式。
可能有的人會(huì)想如果使重心和側(cè)傾軸重合那么就不會(huì)有側(cè)傾力矩了因此就沒(méi)有側(cè)傾了，或者更進(jìn)一步想如果側(cè)傾軸在重心之上那么側(cè)傾力矩就會(huì)使汽車像摩托車一樣向里傾斜。事實(shí)上設(shè)計(jì)一種懸架布置實(shí)現(xiàn)這些是很可能。如果這樣的話，為什么我們需要主動(dòng)懸架系統(tǒng)呢？因?yàn)槿绻覀冇幂^高的側(cè)傾軸的話，那么懸架布置在轉(zhuǎn)彎時(shí)將會(huì)提高，這是以前一些擺動(dòng)臂設(shè)計(jì)的經(jīng)驗(yàn)。
很重要的一點(diǎn)需要注意，一個(gè)經(jīng)常被誤解的問(wèn)題，就是不管懸架設(shè)計(jì)所允許的擺動(dòng)角度范圍，實(shí)際重量轉(zhuǎn)移的程度時(shí)不變的。這只受運(yùn)動(dòng)軌跡、重心和側(cè)向加速度的影響。
所以如同在機(jī)械中的大多數(shù)設(shè)計(jì)特征一樣，側(cè)傾軸線的位置的選擇時(shí)一個(gè)平衡：太低的話我們得到過(guò)度側(cè)傾，太高的話其它的不舒服的操縱特性將表形出來(lái)。實(shí)際上，不同型號(hào)的車這個(gè)平衡是不一樣的但是總是有側(cè)傾發(fā)生。降低重心是另一個(gè)技術(shù)上可能減小側(cè)傾力矩，但是這只能在一個(gè)特定的范圍內(nèi)做到，因?yàn)楸匦枇舫鲎銐虻目臻g讓乘客下車。
這種平衡留下的側(cè)傾力矩必需有汽車彈簧來(lái)抵消，這使我們認(rèn)識(shí)側(cè)傾剛度。這個(gè)名詞被定義為側(cè)傾角等于側(cè)傾力矩除以側(cè)傾剛度。剛性彈簧很顯然減少側(cè)傾因此增加側(cè)傾剛度，但是如果這是選擇彈簧彈性的標(biāo)準(zhǔn)我們將會(huì)很不舒服，在正常的不平的公路上，所以發(fā)展抗側(cè)傾的桿來(lái)緩解這種情況。
抗側(cè)傾的桿是扭轉(zhuǎn)桿（扭轉(zhuǎn)彈簧）連到懸架系統(tǒng)上在汽車的兩邊這樣車輪就可以表現(xiàn)不受阻礙的兩個(gè)碰撞，就像橫穿道路的脊。但是如果車輪試著獨(dú)立運(yùn)動(dòng)，像一個(gè)輪子碰撞，或者當(dāng)汽車側(cè)傾時(shí)向相反的方向那么抗側(cè)傾桿就抵抗這種趨勢(shì)。側(cè)傾就將會(huì)減少但是舒適性變差因?yàn)閷?shí)際車輪的彈性變硬在單獨(dú)的一個(gè)車輪碰撞時(shí)，雖然聯(lián)合兩個(gè)車輪的彈簧特性在干擾處沒(méi)有改變。
又一個(gè)平衡在最小的側(cè)傾需要和很好的道路沖擊感必需滿足。側(cè)傾保護(hù)桿，不像彈簧是等幅運(yùn)動(dòng)的（理論上阻尼可以合并，雖然制造商通常認(rèn)為那是沒(méi)價(jià)值的）。這是另一個(gè)原因限制抗側(cè)傾桿的作用，因?yàn)槿绻@個(gè)桿過(guò)硬就會(huì)產(chǎn)生擺動(dòng)。
很明顯汽車不足/過(guò)多轉(zhuǎn)向特性可以在本質(zhì)上改變通過(guò)協(xié)調(diào)彈性和抗側(cè)傾桿的剛度，改變兩邊的側(cè)傾剛度
當(dāng)汽車作為一個(gè)整體有一個(gè)側(cè)傾剛度，這由獨(dú)立的前后側(cè)傾剛度，它們可能差很多。例如，讓我們考慮一個(gè)軸繞懸架轉(zhuǎn)動(dòng)在其中點(diǎn)，沒(méi)有任何行駛的彈性。這種布置看似不可能，你能在一些牽引車上看到，因?yàn)樗鼈冇珊玫牡孛孢m應(yīng)能力。現(xiàn)在，因?yàn)閼壹苁顷P(guān)于軸的轉(zhuǎn)動(dòng)點(diǎn)完全自由轉(zhuǎn)動(dòng)的，那么沒(méi)有側(cè)傾剛度在機(jī)械的末端被提供所以所有所需的剛度必需在另一端可用。
缺少任何側(cè)傾剛度意味著車身側(cè)傾不能引起任何重量轉(zhuǎn)移到外側(cè)車輪上，因此作為總的重量轉(zhuǎn)移必需在任何情況下一致，另一端必需明顯的成比例的增加
輪胎有一個(gè)有趣的特性是雖然它們能夠承受更大的離心力當(dāng)它們能夠承受更大的垂直載荷，但這不是成比例增加的。換句話說(shuō)，共同作用的摩擦力在更多的重量壓在車輪上時(shí)被減小了。實(shí)際上這意味著重量轉(zhuǎn)移減少了汽車一端車輪增加的離心力?，F(xiàn)在正如我們所看到的，重量轉(zhuǎn)移在汽車的任何一邊能夠由選擇這邊或另一邊活捉或者兩邊的側(cè)傾剛度控制在一定范圍內(nèi)。因此輪胎側(cè)偏角需要產(chǎn)生合適的離心力來(lái)適應(yīng)車輪彈性的改變，這樣給我們了選擇不足/過(guò)多轉(zhuǎn)向特性。
阻尼器也有參與極端復(fù)雜的的相互關(guān)聯(lián)的各種作用在汽車上的力。在剛開(kāi)始變形到完全變形的這個(gè)過(guò)程中，減震器將影響動(dòng)力側(cè)傾剛度。因?yàn)闇p震器只在懸架真正運(yùn)動(dòng)時(shí)起作用，但是它們?cè)谄嚪€(wěn)定轉(zhuǎn)動(dòng)時(shí)不起作用。
所以現(xiàn)在你知道了為什么賽車手們花大量的時(shí)間在他們的賽車上設(shè)置懸架的剛度，當(dāng)初看之下懸架只是防沖擊的墊子。許多競(jìng)賽車都在運(yùn)動(dòng)中改變側(cè)傾穩(wěn)定桿剛度的能力，不僅使其更快的完成期望的表現(xiàn)也能允許對(duì)比賽時(shí)輪胎的磨損和燃油重量的減少進(jìn)行調(diào)節(jié)。
所以主動(dòng)懸架是怎么改進(jìn)這種情況的？電腦程序控制系統(tǒng)能做到，例如分配到前后的側(cè)傾剛度。
假定，系統(tǒng)設(shè)置為零側(cè)傾(這沒(méi)準(zhǔn)就是未來(lái)制造商的目的)那么實(shí)現(xiàn)幾何側(cè)傾中心等的關(guān)聯(lián)是很有趣的。根本上如果我們沒(méi)有側(cè)傾那么側(cè)傾軸就變得不恰當(dāng)了，正如需要懸架連接布置來(lái)試著在轉(zhuǎn)彎側(cè)傾時(shí)保持外側(cè)車輪直立而不是在所有的情況下。也許主動(dòng)懸架意味著回到了平行的等長(zhǎng)雙橫臂或者單橫臂系統(tǒng)。通常，這些設(shè)計(jì)被否定了因?yàn)楹芏嗟膫?cè)傾中心位置，和因?yàn)橥鈨A角隨車身側(cè)傾角變化而變化，汽車總是平行橫臂。直線行駛穩(wěn)定性將會(huì)被提高因?yàn)闆_擊引起的車輪側(cè)偏不會(huì)引起任何的由于改變車輪外傾角所引起的沖擊轉(zhuǎn)向。如果用我們已經(jīng)知道的通常的彈簧和阻尼減震器來(lái)完成不是不可能的話，那是令人滿意的很難做到的情況。
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