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Car suspension
Car suspension
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Part of car suspension system consists of shock absorber, axle, frame and spring
Part of car front suspension and steering mechanism: tie rod, steering arm, king pin axis (using ball joints).
Van Diemen RF01 racing car suspension

Suspension is the system of tires, tire air, springs, shock absorbers and linkages that connects a vehicle to its wheels and allows relative motion between the two.[1] Suspension systems must support both road holding/handling and ride quality,[2] which are at odds with each other. The tuning of suspensions involves finding the right compromise. The suspension is crucial for maintaining consistent contact between the road wheel and the road surface, as all forces exerted on the vehicle by the road or ground are transmitted through the tires' contact patches. The suspension also protects the vehicle itself and any cargo or luggage from damage and wear. The design of front and rear suspension of a car may be different.

History

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American stagecoach showing thoroughbrace suspension—note the black straps under the curved body of the coach

An early form of suspension on ox-drawn carts had the platform swing on iron chains attached to the wheeled frame of the carriage. This system remained the basis for most suspension systems until the turn of the 19th century, although the iron chains were replaced with the use of leather straps called thoroughbraces by the 17th century. No modern automobiles have used the thoroughbrace suspension system.

By approximately 1750, leaf springs began appearing on certain types of carriage, such as the Landau.[3]

By the middle of the 19th century, elliptical springs might additionally start to be used on carriages.

Modern suspension

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The front suspension components of a Ford Model T.

Automobiles were initially developed as self-propelled versions of horse-drawn vehicles. However, horse-drawn vehicles had been designed for relatively slow speeds, and their suspension was not well suited to the higher speeds permitted by the internal combustion engine.

The first workable spring-suspension required advanced metallurgical knowledge and skill, and only became possible with the advent of industrialisation. Obadiah Elliott registered the first patent for a spring-suspension vehicle; each wheel had two durable steel leaf springs on each side and the body of the carriage was fixed directly to the springs which were attached to the axles. Within a decade, most British horse carriages were equipped with springs; wooden springs in the case of light one-horse vehicles to avoid taxation, and steel springs in larger vehicles. These were often made of low-carbon steel and usually took the form of multiple layer leaf springs.[4]

Leaf springs have been around since the early Egyptians. Ancient military engineers used leaf springs in the form of bows to power their siege engines, with little success at first. The use of leaf springs in catapults was later refined and made to work years later. Springs were not only made of metal; a sturdy tree branch could be used as a spring, such as with a bow. Horse-drawn carriages and Ford Model T used this system, and it is still used today in larger vehicles, mainly mounted in the rear suspension.[5]

Leaf springs were the first modern suspension system, and, along with advances in the construction of roads, heralded the single greatest improvement in road transport until the advent of the automobile.[6] The British steel springs were not well-suited for use on America's rough roads of the time, so the Abbot-Downing Company of Concord, New Hampshire re-introduced leather strap suspension, which gave a swinging motion instead of the jolting up-and-down of spring suspension.

Henri Fournier on his uniquely damped and racewinning 'Mors Machine', photo taken 1902

In 1901, Mors of Paris first fitted an automobile with shock absorbers. With the advantage of a damped suspension system on his 'Mors Machine', Henri Fournier won the prestigious Paris-to-Berlin race on 20 June 1901. Fournier's superior time was 11 hours 46 minutes and 10 seconds, while the best competitor was Léonce Girardot in a Panhard with a time of 12 hours, 15 minutes, and 40 seconds.[7]

Coil springs first appeared on a production vehicle in 1906 in the Brush Runabout made by the Brush Motor Company. Today, coil springs are used in most cars.

In 1920, Leyland Motors used torsion bars in a suspension system.

In 1922, independent front suspension was pioneered on Lancia Lambda, and became more common in mass market cars from 1932.[8] Today, most cars have independent suspension on all four wheels.

The part on which pre-1950 springs were supported is called a dumb iron.

In 2002, a new passive suspension component, the inerter, was invented by Malcolm C. Smith. This has the ability to increase the effective inertia of wheel suspension using a geared flywheel, but without adding significant mass. It was initially employed in Formula One in secrecy, but has since spread to wider motorsport.

Difference between rear suspension and front suspension

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For front-wheel drive cars, rear suspension has few constraints, and a variety of beam axles and independent suspensions are used. For rear-wheel drive cars, rear suspension has many constraints, and the development of the superior, but more expensive independent suspension layout has been difficult.[citation needed]

History

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Henry Ford's Model T used a torque tube to restrain this force, for his differential was attached to the chassis by a lateral leaf spring and two narrow rods. The torque tube surrounded the true driveshaft and exerted the force to its ball joint at the extreme rear of the transmission, which was attached to the engine. A similar method like this was used in the late 1930s by Buick and by Hudson's bathtub car in 1948, which used helical springs that could not take fore-and-aft thrust.

The Hotchkiss drive, invented by Albert Hotchkiss, was the most popular rear suspension system used in American cars from the 1930s to the 1970s. The system uses longitudinal leaf springs attached both forward and behind the differential of the live axle. These springs transmit torque to the frame. Although scorned by many European car makers of the time, it was accepted by American car makers, because it was inexpensive to manufacture. Also, the dynamic defects of this design were suppressed by the enormous weight of U.S. passenger vehicles before the implementation of the Corporate Average Fuel Economy (CAFE) standard.

Another Frenchman invented the De Dion tube, which is sometimes called "semi-independent". Like true independent rear suspension, this employs two universal joints, or their equivalent from the centre of the differential to each wheel. But the wheels cannot entirely rise and fall independently of each other; they are tied by a yoke that goes around the differential, below and behind it. This method has had little use in the United States. Its use around 1900 was probably due to the poor quality of tires, which wore out quickly. By removing a good deal of unsprung weight, as independent rear suspensions do, it made them last longer.[citation needed]

Rear-wheel drive vehicles today frequently use a fairly complex fully-independent, multi-link suspension to locate the rear wheels securely, while providing decent ride quality.[citation needed]

Spring, wheel, and roll rates

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Citroën BX Hydropneumatic suspension - maximum to minimum demonstration

Spring rate

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The spring rate (or suspension rate) is a component in setting the vehicle's ride height or its location in the suspension stroke. When a spring is compressed or stretched, the force it exerts, is proportional to its change in length. The spring rate or spring constant of a spring is the change in the force it exerts, divided by the change in deflection of the spring. Vehicles that carry heavy loads, will often have heavier springs to compensate for the additional weight that would otherwise collapse a vehicle to the bottom of its travel (stroke). Heavier springs are also used in performance applications, where the loading conditions experienced are more significant.

Springs that are too hard or too soft cause the suspension to become ineffective – mostly because they fail to properly isolate the vehicle from the road. Vehicles that commonly experience suspension loads heavier than normal, have heavy or hard springs, with a spring rate close to the upper limit for that vehicle's weight. This allows the vehicle to perform properly under a heavy load, when control is limited by the inertia of the load. Riding in an empty truck meant for carrying loads can be uncomfortable for passengers, because of its high spring rate relative to the weight of the vehicle. A race car could also be described as having heavy springs, and would also be uncomfortably bumpy. However, even though we say they both have heavy springs, the actual spring rates for a 2,000 lb (1,000 kg) racecar and a 10,000 lb (5,000 kg) truck are very different. A luxury car, taxi, or passenger bus would be described as having soft springs, for the comfort of their passengers or driver. Vehicles with worn-out or damaged springs ride lower to the ground, which reduces the overall amount of compression available to the suspension, and increases the amount of body lean. Performance vehicles can sometimes have spring rate requirements other than vehicle weight and load.

Wheel rate

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Wheel rate is the effective spring rate when measured at the wheel, as opposed to simply measuring the spring rate alone.

Wheel rate is usually equal to or considerably less than the spring rate. Commonly, springs are mounted on control arms, swing arms or some other pivoting suspension member. Consider the example above, where the spring rate was calculated to be 500 lbs/inch (87.5 N/mm), if one were to move the wheel 1 in (2.5 cm) (without moving the car), the spring more than likely compresses a smaller amount. If the spring moved 0.75 in (19 mm), the lever arm ratio would be 0.75:1. The wheel rate is calculated by taking the square of the ratio (0.5625) times the spring rate, thus obtaining 281.25 lbs/inch (49.25 N/mm). The ratio is squared because it has two effects on the wheel rate: it applies to both the force and the distance traveled.

Wheel rate on independent suspension is fairly straightforward. However, special consideration must be taken with some non-independent suspension designs. Take the case of the straight axle. When viewed from the front or rear, the wheel rate can be measured by the means above. Yet, because the wheels are not independent, when viewed from the side under acceleration or braking, the pivot point is at infinity (because both wheels have moved) and the spring is directly inline with the wheel contact patch. The result is often, that the effective wheel rate under cornering is different from what it is under acceleration and braking. This variation in wheel rate may be minimised by locating the spring as close to the wheel as possible.

Wheel rates are usually summed and compared with the sprung mass of a vehicle to create a "ride rate" and the corresponding suspension natural frequency in ride (also referred to as "heave"). This can be useful in creating a metric for suspension stiffness and travel requirements for a vehicle.

Roll rate

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Roll rate is analogous to a vehicle's ride rate, but for actions that include lateral accelerations, causing a vehicle's sprung mass to roll. It is expressed as torque per degree of roll of the vehicle sprung mass. It is influenced by factors including but not limited to vehicle sprung mass, track width, CG height, spring and damper rates, roll centre heights of front and rear, anti-roll bar stiffness and tire pressure/construction. The roll rate of a vehicle can, and usually, does differ front-to-rear, which allows for the tuning ability of a vehicle for transient and steady-state handling. The roll rate of a vehicle does not change the total amount of weight transfer on the vehicle, but shifts the speed and percentage of weight transferred on a particular axle to another axle through the vehicle chassis. Generally, the higher the roll rate on an axle of a vehicle, the faster and higher percentage the weight transfer on that axle.[citation needed]

By 2021, some vehicles were offering dynamic roll control with ride-height adjustable air suspension and adaptive dampers.[9]

Roll couple percentage

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Roll couple percentage is a simplified method of describing lateral load transfer distribution front to rear, and subsequently handling balance. It is the effective wheel rate, in roll, of each axle of the vehicle as a ratio of the vehicle's total roll rate. It is commonly adjusted through the use of anti-roll bars, but can also be changed through the use of different springs.

Weight transfer

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Weight transfer during cornering, acceleration, or braking is usually calculated per individual wheel, and compared with the static weights for the same wheels.

The total amount of weight transfer is only affected by four factors: the distance between wheel centers (wheelbase in the case of braking, or track width in the case of cornering), the height of the center of gravity, the mass of the vehicle, and the amount of acceleration experienced.

The speed at which weight transfer occurs, as well as through which components it transfers, is complex, and is determined by many factors; including, but not limited to: roll center height, spring and damper rates, anti-roll bar stiffness, and the kinematic design of suspension links.

In most conventional applications, when weight is transferred through intentionally compliant elements, such as springs, dampers, and anti-roll bars, the weight transfer is said to be "elastic", while the weight which is transferred through more rigid suspension links, such as A-arms and toe links, is said to be "geometric".

Unsprung weight transfer

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Unsprung weighttransfer is calculated based on weight of the vehicle's components that are not supported by the springs. This includes tires, wheels, brakes, spindles, half the control arm's weight, and other components. These components are then (for calculation purposes) assumed to be connected to a vehicle with zero sprung weight. They are then put through the same dynamic loads.

The weight transfer for cornering in the front would be equal to the total unsprung front weight times the G-force times the front unsprung center of gravity height divided by the front track width. The same is true for the rear.

Sprung weight transfer

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Sprung weight transfer is the weight transferred by only the weight of the vehicle resting on its springs, and not by total vehicle weight. Calculating this requires knowing the vehicle's sprung weight (total weight less the unsprung weight), the front and rear roll center heights, and the sprung center of gravity height (used to calculate the roll moment arm length). Calculating the front and rear sprung weight transfer will also require knowing the roll couple percentage.

The roll axis is the line through the front and rear roll centers that the vehicle rolls around during cornering. The distance from this axis to the sprung center of gravity height is the roll moment arm length. The total sprung weight transfer is equal to the G-force times the sprung weight times the roll moment arm length divided by the effective track width. The front sprung weight transfer is calculated by multiplying the roll couple percentage times the total sprung weight transfer. The rear is the total minus the front transfer.

Jacking forces

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Jacking forces are the sum of the vertical force components experienced by suspension links. The resultant force acts to lift the sprung mass, if the roll center is above ground, or compress it, if underground. Generally, the higher the roll center, the more jacking force is experienced.

Other properties

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Travel

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Travel is the measure of distance from the bottom of the suspension stroke (such as when the vehicle is on a jack, and the wheel hangs freely) to the top of the suspension stroke (such as when the vehicle's wheel can no longer travel in an upward direction toward the vehicle). Bottoming or lifting a wheel can cause serious control problems, or directly cause damage. "Bottoming" can be caused by the suspension, tires, fenders, etc. running out of space to move, or the body or other components of the car hitting the road. Control problems caused by lifting a wheel are less severe, if the wheel lifts when the spring reaches its unloaded shape than they are, if travel is limited by contact of suspension members (See Triumph TR3B.)

Many off-road vehicles, such as desert racers, use straps called "limiting straps" to limit the suspensions' downward travel to a point within safe limits for the linkages and shock absorbers. This is necessary, since these trucks are intended to travel over very rough terrain at high speeds, and even become airborne at times. Without something to limit the travel, the suspension bushings would take all the force, when suspension reaches "full droop", and it can even cause the coil springs to come out of their "buckets", if they are held in by compression forces only. A limiting strap is a simple strap, often from nylon of a predetermined length, that stops downward movement at a pre-set point before theoretical maximum travel is reached. The opposite of this is the "bump-stop", which protects the suspension and the vehicle (as well as the occupants) from the violent "bottoming" of the suspension, caused when an obstruction (or a hard landing) causes suspension to run out of upward travel without fully absorbing the energy of the stroke. Without bump-stops, a vehicle that "bottoms out", will experience a very hard shock when the suspension contacts the bottom of the frame or body, which is transferred to the occupants and every connector and weld on the vehicle. Factory vehicles often come with plain rubber "nubs" to absorb the worst of the forces, and insulate the shock. A desert race vehicle, which must routinely absorb far higher impact forces, might be provided with pneumatic or hydro-pneumatic bump-stops. These are essentially miniature shock absorbers (dampers) that are fixed to the vehicle in a location, such, that the suspension will contact the end of the piston when it nears the upward travel limit. These absorb the impact far more effectively than a solid rubber bump-stop will, essential, because a rubber bump-stop is considered a "last-ditch" emergency insulator for the occasional accidental bottoming of the suspension; it is entirely insufficient to absorb repeated and heavy bottoming, such as a high-speed off-road vehicle encounters.

Damping

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Damping is the control of motion or oscillation, as seen with the use of hydraulic gates and valves in a vehicle's shock absorber. This may also vary, intentionally or unintentionally. Like spring rate, the optimal damping for comfort may be less, than for control.

Damping controls the travel speed and resistance of the vehicle's suspension. An undamped car will oscillate up and down. With proper damping levels, the car will settle back to a normal state in a minimal amount of time. Most damping in modern vehicles can be controlled by increasing or decreasing the resistance to fluid flow in the shock absorber.

Camber control

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See dependent and independent below. Camber changes due to wheel travel, body roll and suspension system deflection or compliance. In general, a tire wears and brakes best at -1 to -2° of camber from vertical. Depending on the tire and the road surface, it may hold the road best at a slightly different angle. Small changes in camber, front and rear, can be used to tune handling. Some racecars are tuned with -2 to -7° camber, depending on the type of handling desired, and tire construction. Often, too much camber will result in the decrease of braking performance due to a reduced contact patch size through excessive camber variation in suspension geometry. The amount of camber change in bump is determined by the instantaneous front view swing arm (FVSA) length of suspension geometry, or in other words, the tendency of the tire to camber inward when compressed in bump.

Roll center height

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Roll center height is a product of suspension instant center heights and is a useful metric in analyzing weight transfer effects, body roll and front to rear roll stiffness distribution. Conventionally, roll stiffness distribution is tuned adjusting antiroll bars rather than roll center height (as both tend to have a similar effect on the sprung mass), but the height of the roll center is significant when considering the amount of jacking forces experienced.

Instant center

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Due to the fact that the wheel and tire's motion is constrained by the vehicle's suspension links, the motion of the wheel package in the front view will scribe an imaginary arc in space with an "instantaneous center" of rotation at any given point along its path. The instant center for any wheel package can be found by following imaginary lines drawn through suspension links to their intersection point.

A component of the tire's force vector points from the contact patch of the tire through instant center. The larger this component is, the less suspension motion will occur. Theoretically, if the resultant of the vertical load on the tire and the lateral force generated by it points directly into the instant center, the suspension links will not move. In this case, all weight transfer at that end of the vehicle will be geometric in nature. This is key information used in finding the force-based roll center as well.

In this respect, the instant centers are more important to the handling of the vehicle, than the kinematic roll center alone, in that the ratio of geometric-to-elastic weight transfer is determined by the forces at the tires and their directions in relation to the position of their respective instant centers.

Anti-dive and anti-squat

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Anti-dive and anti-squat are percentages that indicate the degree to which the front dives under braking, and the rear squats under acceleration. They can be thought of as the counterparts for braking and acceleration, as jacking forces are to cornering. The main reason for the difference is due to the different design goals between front and rear suspension, whereas suspension is usually symmetrical between the left and the right of the vehicle.

The method of determining anti-dive or anti-squat depends on whether suspension linkages react to the torque of braking and accelerating. For example, with inboard brakes and half-shaft-driven rear wheels, the suspension linkages do not react, but with outboard brakes and a swing-axle driveline, they do.

To determine the percentage of front suspension braking anti-dive for outboard brakes, it is first necessary to determine the tangent of the angle between a line drawn, in side view, through the front tire patch and the front suspension instant center, and the horizontal. In addition, the percentage of braking effort at the front wheels must be known. Then, multiply the tangent by the front wheel braking effort percentage and divide by the ratio of the center of gravity height to the wheelbase. A value of 50% would mean, that half of the weight transfer to the front wheels; during braking, it is being transmitted through front suspension linkage, and half is being transmitted through front suspension springs.

For inboard brakes, the same procedure is followed, but using the wheel center instead of contact patch center.

Forward acceleration anti-squat is calculated in a similar manner and with the same relationship between percentage and weight transfer. Anti-squat values of 100% and more are commonly used in drag racing, but values of 50% or less are more common in cars that have to undergo severe braking. Higher values of anti-squat commonly cause wheel hop during braking. It is important to note, that the value of 100% means, that all of the weight transfer is being carried through suspension linkage. However, this does not mean that the suspension is incapable of carrying additional loads (aerodynamic, cornering, etc.) during an episode of braking, or forward acceleration. In other words, no "binding" of the suspension is to be implied.[10]

Flexibility and vibration modes of suspension elements

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In some modern cars, flexibility is mainly in rubber bushings, which are subject to decay over time. For high-stress suspensions, such as off-road vehicles, polyurethane bushings are available, which offer more longevity under greater stresses. However, due to weight and cost considerations, structures are not made more rigid than necessary. Some vehicles exhibit detrimental vibrations involving the flexing of structural parts, such as when accelerating while turning sharply. Flexibility of structures, such as frames and suspension links, can also contribute to springing, especially to damping out high-frequency vibrations. The flexibility of wire wheels contributed to their popularity in times when cars had less advanced suspensions.

Load levelling

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Automobiles can be heavily laden with luggage, passengers, and trailers. This loading will cause a vehicle's tail to sink downwards. Maintaining a steady chassis level is essential to achieving the proper handling that the vehicle was designed for. Also, if the car's nose is too elevated when driving at night, oncoming drivers can be blinded by the headlight beam. Self-levelling suspension counteracts this by inflating cylinders in the suspension to lift the chassis higher.[11]

Isolation from high frequency shock

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For most purposes, the weight of suspension components is unimportant. But at high frequencies caused by road surface roughness, the parts isolated by rubber bushings act as a multi-stage filter to suppress noise and vibration better than can be done with only tires and springs. (The springs work mainly in the vertical direction.)

Contribution to unsprung weight and total weight

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These are usually small, except that the suspension is related to whether the brakes and differential(s) are sprung.

This is the main functional advantage of aluminum wheels over steel wheels. Aluminum suspension parts have been used in production cars, and carbon fiber suspension parts are common in racing cars.

Space occupied

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Designs differ as to how much space they take up, and where it is located. It is generally accepted, that MacPherson struts are the most compact arrangement for front-engined vehicles, where space between the wheels is required to place the engine.

Inboard brakes (which reduce unsprung weight) are probably avoided more due to space considerations than to cost.

Force distribution

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The suspension attachment must match the frame design in geometry, strength and rigidity.

Air resistance (drag)

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Certain modern vehicles have height adjustable suspension in order to improve aerodynamics and fuel efficiency. Modern formula cars that have exposed wheels and suspension typically use streamlined tubing rather than simple round tubing for their suspension arms to reduce aerodynamic drag. Also typical is the use of rocker-arm, push rod, or pull rod-type suspensions, that, among other things, place the spring/damper unit inboard and out of the air stream to further reduce air resistance.

Cost

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Production methods improve, but cost is always a factor. The continued use of the solid rear axle, with unsprung differential, especially on heavy vehicles, seems to be the most obvious example.

Springs and dampers

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Most conventional suspensions use passive springs to absorb impacts and dampers (or shock absorbers) to control spring motions.

Some notable exceptions are hydropneumatic systems, which can be treated as an integrated unit of gas spring and damping components, used by the French manufacturer Citroën; and the hydrolastic, hydragas and rubber cone systems used by the British Motor Corporation, most notably on the Mini. A number of different types of each have been used:

Passive suspensions

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Traditional springs and dampers are referred to as passive suspensions — most vehicles are suspended in this manner.

Springs

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Pneumatic spring on a semitrailer

The majority of land vehicles are suspended by steel springs of these types:

Automakers are aware of the inherent limitations of steel springs — that these springs tend to produce undesirable oscillations, and carmakers have developed other types of suspension materials and mechanisms in attempts to improve performance:

Dampers or shock absorbers

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Shock absorbers damp out the (otherwise simple harmonic) motions of a vehicle up and down on its springs. They must also damp out much of the wheel bounce when the unsprung weight of a wheel, hub, axle, and sometimes brakes and the differential bounces up and down on the springiness of a tire.

Semi-active and active suspensions

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If suspension is externally controlled, then it is a semi-active or active suspension — the suspension is reacting to signals from an electronic controller.

For example, a hydropneumatic Citroën will "know" how far off the ground the car is supposed to be, and constantly resets to achieve that level, regardless of load. However, this type of suspension will not instantly compensate for body roll due to cornering. Citroën's system adds about 1% to the cost of the car versus passive steel springs.

Semi-active suspensions include devices, such as air springs and switchable shock absorbers, various self-levelling solutions, as well as systems, like hydropneumatic, hydrolastic, and hydragas suspensions.

Toyota introduced switchable shock absorbers in the 1983 Soarer.[17] Delphi currently sells shock absorbers filled with a magneto-rheological fluid, whose viscosity can be changed electromagnetically — thereby giving variable control without switching valves, which is faster and thus more effective.

Fully active suspension systems use electronic monitoring of vehicle conditions, coupled with the means to change the behavior of vehicle suspension in real time to directly control the motion of the car.

Lotus Cars developed several prototypes from 1982 onwards, and introduced them to Formula One, where they have been fairly effective, but have now been banned.

Nissan introduced low-bandwidth active suspension circa 1990 as an option that added an extra 20% to the price of luxury models. Citroën has also developed several active suspension models (see hydractive). A fully active system from Bose Corporation, announced in 2009, uses linear electric motors[18][19][20][21][22] in place of hydraulic or pneumatic actuators that have generally been used up until recently. Mercedes introduced an active suspension system called Active Body Control in its top-of-the-line Mercedes-Benz CL-Class in 1999.

Several electromagnetic suspensions have also been developed for vehicles. Examples include the electromagnetic suspension of Bose, and the electromagnetic suspension developed by prof. Laurentiu Encica. In addition, the new Michelin wheel with embedded suspension functioning on an electric motor is also similar.[23]

With the help of a control system, various semi-active/active suspensions realize an improved design compromise among different vibration modes of the vehicle; namely: bounce, roll, pitch and warp modes. However, the applications of these advanced suspensions are constrained by cost, packaging, weight, reliability, and/or other challenges.

Interconnected suspensions

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Interconnected suspension, unlike semi-active/active suspensions, could easily decouple different vehicle vibration modes in a passive manner. Interconnections can be realized by various means, such as mechanical, hydraulic, and pneumatic. Anti-roll bars are one of the typical examples of mechanical interconnections, while it has been stated, that fluidic interconnections offer greater potential and flexibility in improving both the stiffness and damping properties.

Considering the considerable commercial potentials of hydro-pneumatic technology (Corolla, 1996), interconnected hydropneumatic suspensions have also been explored in some recent studies, and their potential benefits in enhancing vehicle ride and handling have been demonstrated. The control system can also be used for further improving performance of interconnected suspensions. Apart from academic research, an Australian company Kinetic[24] had some success with various passive or semi-active systems (WRC: three Championships; the Dakar Rally: two Championships; Lexus GX470 2004 as the 4×4 of the year with KDSS; the 2005 PACE award). These systems by Kinetic generally decouple at least two vehicle modes (roll, warp (articulation), pitch, and/or heave (bounce)) to simultaneously control each mode's stiffness and damping by using interconnected shock absorbers, and other methods. In 1999, Kinetic was bought out by Tenneco. Later developments by the Catalan company Creuat have devised a simpler system design based on single-acting cylinders. After some projects on competition, Creuat is active in providing retrofit systems for some vehicle models.

Historically, the first mass-production car with front-to-rear mechanical interconnected suspension was the 1948 Citroën 2CV. Suspension in the 2CV was extremely soft — the longitudinal link was making pitch softer, instead of making roll stiffer. It relied on extreme anti-dive and anti-squat geometries to compensate for that. This resulted in a softer axle-crossing stiffness that anti-roll bars would have otherwise compromised. The leading arm / trailing arm swinging arm, fore-aft linked suspension system, together with in-board front brakes, had a much smaller unsprung weight than existing coil spring or leaf designs. The interconnection transmitted some of the force deflecting a front wheel up over a bump, to push the rear wheel down on the same side. When the rear wheel met that bump a moment later, it did the same in reverse, keeping the car level front to rear. The 2CV had a design brief to be able to be driven at speed over a ploughed field, such as by a farmer transporting chicken eggs. It originally featured friction dampers and tuned mass dampers. Later models had tuned mass dampers at the front with telescopic dampers/shock absorbers front and rear.

British Motor Corporation was also an early adopter of interconnected suspension. A system dubbed Hydrolastic was introduced in 1962 on Morris 1100, and went on to be used on a variety of BMC models. Hydrolastic was developed by suspension engineer Alex Moulton, and used rubber cones as the springing medium (these were first used on the 1959 Mini) with suspension units on each side connected to each other by a fluid-filled pipe. The fluid transmitted the force of road bumps from one wheel to the other (on the same principle as Citroën 2CV's mechanical system described above), and because each suspension unit contained valves to restrict the flow of fluid, also served as a shock absorber.[25] Moulton went on to develop a replacement for Hydrolastic for BMC's successor British Leyland. This system, manufactured under licence by Dunlop in Coventry, called Hydragas, worked with the same principle, but instead of rubber spring units, it used metal spheres divided internally by a rubber diaphragm. The top half contained pressurised gas, and the lower half the same fluid as used on the Hydrolastic system. The fluid transmitted suspension forces between the units on each side, whilst the gas acted as the springing medium through the diaphragm. This is the same principle as the Citroën hydropneumatic system, and provides similar ride quality, but is self-contained, and does not require an engine-driven pump to provide hydraulic pressure. The downside is, that Hydragas is, unlike the Citroën system, not height-adjustable, or self-levelling. Hydragas was introduced in 1973 on Austin Allegro, and was used on several models; the last car to use it being MG F in 2002. The system was changed in favour of coil springs over dampers due to cost reasons towards the end of the vehicle's life. When it was decommissioned in 2006, the Hydragas manufacturing line was over 40 years old.

Some of the last post-war Packard models also featured interconnected suspension.

Types

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Common types seen from behind; in order:
  • Live axle with a Watt's link
  • Sliding pillar
  • Swing axle
  • Double wishbone suspension
  • MacPherson
This diagram is not exhaustive; notably, it excludes elements, such as trailing arm links, and those that are flexible.

Suspension systems can be broadly classified into two subgroups: dependent and independent. These terms refer to the ability of opposite wheels to move independently of each other.[26] A dependent suspension normally has a beam (a simple 'cart' axle) or a (driven) live axle that holds wheels parallel to each other and perpendicular to the axle. When the camber of one wheel changes, the camber of the opposite wheel changes in the same way (by convention, on one side, this is a positive change in the camber, and on the other side, this a negative change). De Dion suspensions are also in this category, as they rigidly connect the wheels together.

Independent suspension allows wheels to rise and fall on their own without affecting the opposite wheel. Suspensions with other devices, such as sway bars that link the wheels in some way, are still classed as independent.

Semi-dependent suspension is a third type. In this case, the motion of one wheel does affect the position of the other, but they are not rigidly attached to each other. Twist-beam rear suspension is such a system.

Dependent suspensions

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Dependent systems may be differentiated by the system of linkages used to locate them, both longitudinally and transversely. Often, both functions are combined in a set of linkages.

Examples of location linkages include:

  • Satchell link
  • Panhard rod
  • Watt's linkage
  • WOBLink
  • Mumford linkage
  • Leaf springs used for location (transverse or longitudinal)
    • Fully elliptical springs usually need supplementary location links, and are no longer in common use
    • Longitudinal semi-elliptical springs used to be common, and are still used in heavy-duty trucks and aircraft. They have the advantage, that the spring rate can easily be made progressive (non-linear).
    • A single transverse leaf spring for both front wheels and/or both back wheels, supporting solid axles, was used by Ford Motor Company, before and soon after World War II, even on expensive models. It had the advantages of simplicity and low unsprung weight (compared to other solid-axle designs).

In a front-engine rear-drive vehicle, dependent rear suspension is either "live-axle" or deDion axle, depending on whether or not differential is carried on the axle. Live-axle is simpler, but unsprung weight contributes to wheel bounce.

Because it assures constant camber, dependent (and semi-independent) suspension is most common on vehicles that need to carry large loads as a proportion of the vehicle's weight, that have relatively soft springs and that do not (for cost and simplicity reasons) use active suspensions. The use of dependent front suspension has become limited to heavier commercial vehicles.

Independent suspensions

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Rear independent suspension on an AWD car.

The variety of independent systems is greater, and includes:

Because the wheels are not constrained to remain perpendicular to a flat road surface in turning, braking, and varying load conditions, control of the wheel camber is an important issue. Swinging-arm was common in small cars that were sprung softly, and could carry large loads, because the camber is independent of load. Some active and semi-active suspensions maintain ride height, and therefore the camber, independent of load. In sports cars, optimal camber change when turning, is more important.

Wishbone and multi-link allow the engineer more control over the geometry, to arrive at the best compromise, than swing axle, MacPherson strut, or swinging arm do; however, the cost and space requirements may be greater.

Semi-trailing arm is in between, being a variable compromise between the geometries of swinging arm and swing axle.

Semi-independent suspension

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In semi-independent suspensions, the wheels of an axle are able to move relative to one another, as in an independent suspension, but the position of one wheel has an effect on the position and attitude of the other wheel. This effect is achieved through the twisting or deflecting of suspension parts under load.

The most common type of semi-independent suspension is the twist beam.

Other instances

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Tilting Suspension System

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The Tilting Suspension System[27] (also known as the Leaning Suspension System) is not a different type or geometry of construction; moreover, it is a technology addition to the conventional suspension system.

This kind of suspension system mainly consists of independent suspension (e.g., MacPherson strut, A-arm (double wishbone)). With the addition of these suspension systems, there is a further tilting or leaning mechanism that connects the suspension system with the vehicle body (chassis).

The tilting suspension system improves stability, traction, the turning radius of a vehicle, and the comfort of riders as well. While turning right or left, passengers or objects on a vehicle feel the G-force or inertial force outward the radius of the curvature, which is why two-wheeler riders (motorbikes) lean towards the center of curvature while turning, which improves stability and decreases the chances of toppling. But vehicles with more than two wheels, and equipped with a conventional suspension system, could not do the same until now, so the passengers feel the outward inertial force, which reduces the stability of riders and their comfort as well. This kind of tilting suspension system is the solution to the problem. If the road does not have super-elevation or banking, it will not affect the comfort with this suspension system, the vehicle tilt and decrease in the height of the center of gravity with an increase in stability. This suspension is also used in fun vehicles.

Some trains also use tilting suspension (Tilting Train) which increases the speed at cornering.

Rocker bogie mechanism

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The rocker-bogie system is a suspension arrangement, in which there are some trailing arms fitted with some idler wheels. Due to articulation between the driving section and the followers, this suspension is very flexible. This kind of suspension is appropriate for extremely rough terrain.

This kind of suspension was used in the Curiosity rover.

Tracked vehicles

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Some vehicles, such as trains, run on long rail tracks fixed to the ground; and some, such as tractors, snow vehicles, and tanks run on continuous tracks that are part of the vehicle. Although either sort helps to smooth the path and reduce ground pressure, many of the same considerations apply.

Armoured fighting vehicle suspension

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This Grant I tank's suspension has road wheels mounted on wheel trucks, or bogies.

Military armoured fighting vehicles (AFVs), including tanks, have specialized suspension requirements. They can weigh more than seventy tons, and are required to move as quickly as possible over very rough or soft ground. Their suspension components must be protected from land mines and antitank weapons. Tracked AFVs can have as many as nine road wheels on each side. Many wheeled AFVs have six or eight large wheels. Some have a Central Tire Inflation System to reduce ground loading on poor surfaces. Some wheels are too big and too confined to turn, so skid steering is used with some wheeled, as well as with tracked vehicles.

The earliest tanks of World War I had fixed suspension with no designed movement whatsoever. This unsatisfactory situation was improved with leaf spring or coil spring suspensions adopted from agricultural, automotive, or railway machinery, but even these had very limited travel.

Speeds increased due to more powerful engines, and the quality of ride had to be improved. In the 1930s, the Christie suspension was developed, which allowed the use of coil springs inside a vehicle's armored hull, by changing the direction of force deforming the spring, using a bell crank. The T-34's suspension was directly descended from Christie designs.

Horstmann suspension was a variation which used a combination of bell crank and exterior coil springs, in use from the 1930s to the 1990s. The bogie, but nonetheless independent, suspensions of M3 Lee/Grant and M4 Sherman vehicles was similar to the Hortsmann type, with suspension sequestered within the track oval.

By World War II, the other common type was torsion bar suspension, getting spring force from twisting bars inside the hull — this sometimes had less travel than the Christie type, but was significantly more compact, allowing more space inside the hull, with the consequent possibility to install larger turret rings, and thus, heavier main armament. Torsion-bar suspension, sometimes including shock absorbers, has been the dominant heavy armored vehicle suspension since World War II. Torsion bars may take space under or near the floor, which may interfere with making the tank low to reduce exposure.

As with cars, wheel travel and spring rate affect the bumpiness of ride, and the speed at which rough terrain can be negotiated. It may be significant, that a smooth ride, which is often associated with comfort, increases the accuracy when firing on the move. It also reduces shock on optics and other equipment. The unsprung weight and track link weight may limit speed on roads, and can affect the useful lifetime of the vehicle's track, and its other components.

Most German WWII half-tracks and their tanks introduced during the war, such as the Panther tank, had overlapping and sometimes interleaved road wheels to distribute the load more evenly on the tank's track, and therefore on the ground. This apparently made a significant contribution to speed, range and track life, as well as providing a continuous band of protection. It has not been used since the end of that war, probably due to the maintenance requirements of more complicated mechanical parts working in mud, sand, rocks, snow, and ice; as well as due to cost. Rocks and frozen mud often got stuck between the overlapping wheels, which could prevent them from turning, or would cause damage to the road wheels. If one of the interior road wheels were damaged, it would require other road wheels to be removed in order to access the damaged road wheel, making the process more complicated and time-consuming.[28]

See also

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References

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Further reading

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Revisions and contributorsEdit on WikipediaRead on Wikipedia
from Grokipedia
The suspension of an automobile consists of the mechanical components that connect the wheels to the vehicle's frame or body, allowing relative motion between them while keeping the wheels in contact with surface. This primarily functions to absorb and cushion shock loads from road irregularities, dampen resulting oscillations for stability, and enhance overall ride comfort, handling, and safety. By isolating road disturbances from the vehicle's occupants and maintaining traction, it plays a critical role in , influencing acceleration, braking, and cornering performance. Key elements of the suspension include springs, which store and release elastic energy to support the vehicle's weight and absorb impacts; shock absorbers (or dampers), hydraulic devices that resist spring motion to prevent excessive bouncing; and linkages such as control arms, knuckles, and sway bars that guide wheel movement and distribute forces. Suspension designs vary widely to balance competing goals like comfort and sporty handling: dependent systems, such as solid beam axles with leaf springs, provide durability for heavy loads but limit independent wheel motion; independent systems, including the (introduced in 1947) and double wishbone, allow each wheel to respond separately to road conditions for improved stability and ride quality. Modern advancements incorporate active and semi-active technologies, such as adjustable dampers and air springs, to dynamically adapt to driving conditions, optimizing performance across diverse terrains while meeting regulatory standards for emissions and . In electric vehicles, suspensions are adapted to handle heavy battery packs and optimize range and stability. These evolutions stem from ongoing efforts to refine , materials, and control systems, ensuring suspensions contribute to and reduced wear on tires and other components.

Fundamentals

Purpose and Functions

The car suspension system consists of the mechanical components that connect a vehicle's wheels to its or body, permitting relative motion between them while ensuring continuous contact with the road surface. This design allows the wheels to follow road contours independently of the vehicle's body, maximizing friction for traction and stability. Its core functions include absorbing shocks and vibrations from road irregularities to enhance passenger comfort and protect the from damage, maintaining proper for effective and directional control, supporting the vehicle's weight under static and dynamic loads, and minimizing body roll during cornering to preserve handling balance. By controlling vertical wheel motion, the suspension also optimizes -road interaction, which directly influences braking efficiency through consistent contact patches and acceleration performance by sustaining traction during power delivery. The suspension isolates the sprung mass—the portion of the vehicle above the system—from road disturbances.

Sprung and Unsprung Mass

In , the vehicle's mass is divided into sprung mass and unsprung mass to analyze suspension dynamics. Sprung mass encompasses the portions of the vehicle supported by the suspension system, including the , body, , transmission, passengers, and cargo. Unsprung mass, by contrast, includes components not isolated by the suspension, such as the wheels, tires, assemblies, axles, and certain suspension linkages like control arms and hubs. This distinction is crucial because the suspension primarily isolates the sprung mass from road irregularities, while the unsprung mass directly encounters them. The level of unsprung mass significantly influences ride quality and vehicle traction. Higher unsprung mass amplifies road-induced vibrations transmitted to the sprung mass, resulting in increased harshness and reduced comfort over uneven surfaces. It also diminishes tire-road contact by making it harder for the suspension to maintain adherence during dynamic maneuvers, thereby lowering traction and overall handling responsiveness. Conversely, lowering unsprung mass allows the suspension to react more swiftly to road inputs, improving isolation of the sprung mass and enhancing both ride smoothness and grip. Calculating sprung mass involves subtracting the unsprung mass from the total vehicle mass. For precision, engineers determine unsprung mass per corner by summing components such as the -tire assembly (typically 40-60 pounds per corner), hardware, wheel bearings, knuckles, half the weight of springs and shocks, and relevant or differential portions (total unsprung typically 70-120 pounds per corner). The resulting sprung mass per corner is then used for suspension tuning, ensuring the system effectively supports and isolates the vehicle's primary load. Minimizing unsprung is a key design priority in , particularly for improving handling precision, acceleration efficiency, and fuel economy by reducing the energy required to move these components. In sports cars, where performance demands are high, this often involves using lightweight materials like aluminum alloys for wheels and control arms or carbon fiber for brake components to achieve a higher sprung-to-unsprung ratio. For instance, race cars, which share design principles with production sports vehicles, have demonstrated measurable gains in cornering speeds and stability through unsprung reductions of approximately 5% via optimized uprights and hubs. Such efforts enhance overall vehicle without compromising structural integrity.

Historical Development

Early Innovations

The origins of car suspension systems trace back to pre-automotive horse-drawn carriages, where innovations in spring technology addressed the challenges of uneven travel. Leaf springs, composed of layered, curved steel plates, emerged in the for basic vehicle support, but their modern form was revolutionized by Elliott's 1804 British patent for mounting carriage bodies directly on elliptic springs. This design used two semi-elliptic springs positioned opposite each other to form a full ellipse, shackled to the axles, which lightened the overall weight, improved load distribution, and enhanced ride smoothness compared to earlier leather-strap or perch-based suspensions. These elliptic suspensions became standard on 19th-century coaches and buggies, prioritizing resilience on cobblestone and dirt paths while reducing the need for bulky undercarriage supports. As automobiles emerged in the late , early designers faced significant challenges from rudimentary road infrastructure, which often consisted of deeply rutted dirt tracks or poorly maintained gravel surfaces. This environment demanded rigid suspension designs focused on durability and structural integrity over passenger comfort, as softer systems risked rapid wear, frequent breakdowns, and safety hazards from component failure under constant jolts. Stiff, high-mounted axles with minimal articulation were common to protect vital elements, though they transmitted harsh vibrations to occupants, limiting early vehicles to low speeds and short distances. The transition to motorized vehicles adapted carriage principles directly, with Karl Benz's groundbreaking 1885 Patent-Motorwagen incorporating a rigid rear suspended by elliptic leaf springs, providing essential isolation between the and road imperfections in the world's first practical automobile. By the early , key inventions refined these basics: the 1903 Runabout employed a solid front with a transverse half-elliptic leaf spring, offering simple, cost-effective compliance for emerging . Meanwhile, H.F.S. Morgan's 1910 introduced the sliding pillar front suspension, where vertical pillars guided stub s independently with coil springs, allowing better wheel travel and handling on imperfect roads without complex linkages. Into the 1910s, full-elliptic springs gained widespread adoption for their superior articulation and load-handling, as evidenced by vehicles like the 1910 Paige-Detroit, which paired full-elliptic rear springs with semi-elliptic fronts to deliver a compliant ride suited to expanding automobile use. This configuration, directly inherited from carriage elliptic designs, marked a pivotal shift toward balancing durability with improved comfort as roads began gradual modernization.

Evolution to Modern Systems

The 1930s marked significant breakthroughs in independent suspension designs, moving away from rigid axles toward systems that improved ride quality and handling. The , introduced in 1934, was the first mass-produced European car to feature four-wheel using torsion bars, enabling better road holding and comfort on uneven surfaces. Similarly, the Mercedes-Benz 170H, launched in 1936 as a rear-engine compact model, incorporated independent rear suspension with swing axles and coil springs, which provided smoother articulation compared to contemporary leaf-spring setups, though it struggled with oversteer tendencies. Post-World War II developments in the accelerated the adoption of and simplified independent front suspensions, prioritizing cost-effective manufacturing without sacrificing performance. Ford pioneered the widespread use of the in its British Consul and Zephyr models starting in late 1950, integrating a over a telescopic damper to create a compact, lightweight system that enhanced ride compliance and reduced unsprung mass. This design quickly proliferated across Ford's lineup by the late , influencing global by balancing simplicity with improved geometry control. From the through the , suspension evolved toward multi-link configurations and electronic integration, enabling precise wheel control and adaptive responses to driving conditions. Multi-link systems, originating from Mercedes-Benz's 1969 C111 prototype, entered production in the 1980s with the W201 190 series' five-link rear setup in 1982, using multiple control arms to optimize camber and during cornering for superior handling in luxury sedans. Electronic aids emerged in the , with semi-active dampers allowing real-time damping adjustments via sensors and actuators, as seen in systems that improved stability and comfort in vehicles like Mercedes models. In the , the rise of electric vehicles integrated regenerative into suspension designs, capturing vibrational energy to recharge batteries and enhance efficiency. These systems, often hydraulic or electromagnetic, harvested up to 400 watts from road vibrations in passenger cars, as demonstrated in prototypes and early EV applications that combined with tunable . By 2025, adaptive air suspensions in luxury EVs like the Plaid exemplified this trend, featuring electronically controlled air springs that adjust height and firmness for optimized , ride quality, and handling during high-performance driving.

Kinematic Properties

Suspension Geometry Basics

Suspension geometry refers to the spatial arrangement of components in a vehicle's suspension system that governs wheel alignment, motion paths, and interaction with the road surface. This geometry is crucial for ensuring proper tire contact, response, and overall vehicle handling by controlling parameters such as wheel angles during straight-line travel, braking, acceleration, and cornering. Key alignment angles include , kingpin inclination, and , which influence stability and effort, while optimizes wheel angles during turns. Caster is the angle between the steering axis and the vertical plane when viewed from the side of the , typically positive when the top of the kingpin is tilted rearward to provide self-centering and straight-line stability. Kingpin inclination (KPI), viewed from the front, is the angle between the steering axis and the vertical, which helps reduce effort and by allowing the wheel to pivot around a point closer to the centerline. , the lateral distance at ground level between the center and the projection of the axis, affects torque and stability; a small or zero minimizes unwanted inputs from braking or forces. ensures that during a turn, the inner wheel steers at a sharper than the outer wheel, allowing both to follow concentric arcs around the same turning , which is achieved through the linkage of arms and tie rods in a four-bar mechanism. The instant center is the theoretical point where the extended lines of the suspension links intersect, defining the instantaneous axis of for the relative to the and constraining its motion to approximate a . For the vehicle as a whole, the is the point where the lines connecting the instant centers of the left and right wheels intersect the vehicle's longitudinal centerline; it represents the height about which the sprung mass rolls during cornering without lateral translation of the chassis. In basic kinematic diagrams, the roll axis is the connecting the front and rear roll centers, which determines the path of body roll and contributes to vehicle stability by influencing how lateral forces are transmitted to the chassis during maneuvers. These geometric elements directly impact handling through changes in wheel alignment during suspension travel. Toe change refers to the variation in the wheel's toe angle (the angle between the wheel's plane and the vehicle's centerline) as the suspension compresses or extends, which can either stabilize or destabilize the vehicle if not optimized. Camber gain is the alteration in the wheel's camber angle (tilt from vertical) during cornering or body roll, where a desirable negative camber gain maintains the tire's contact patch flat against the road for maximum grip. Proper tuning of these parameters enhances cornering performance without excessive tire wear.

Camber Control and Roll Centers

Camber control encompasses the suspension geometry configurations designed to maintain optimal camber angles under dynamic loads, particularly during cornering, to maximize -road contact and grip. Negative camber, with the top tilted inward, counters the outward lean induced by body roll, ensuring even loading on the outside . This is achieved through camber gain mechanisms in linkages like double wishbones, where vertical travel induces progressive negative camber changes, typically targeting 0.6–1.0 degrees per degree of roll for balanced handling. Anti-dive geometry contributes to camber control by minimizing front-end pitch under braking, which otherwise alters camber unfavorably; it directs braking torque through the suspension arms to a virtual pivot point above the wheel center, reducing dive and preserving camber stability. In rear suspensions, anti-squat geometry similarly counters acceleration-induced pitch by aligning drive forces to limit squat, maintaining consistent camber for traction. These setups involve angling control arms so that resultant force lines intersect near the vehicle's center of gravity height, with typical anti-dive values of 20–50% to balance stability without excessive harshness. The represents the instantaneous point about which the vehicle rolls under lateral forces, calculated kinematically as the intersection of force lines extending from each wheel's instant center—the point of zero wheel velocity during motion—to the tire-ground . This intersection defines the roll axis when connecting front and rear roll centers. In symmetric suspensions like double wishbones, the roll center height is determined geometrically from the positions of the instant centers and contact patches. This height directly influences load transfer; a lower roll center height increases the moment arm from the center of gravity to the roll axis, directing more lateral load through the compliant suspension elements rather than rigid , which enhances tunable handling but amplifies body roll. Design trade-offs in roll center placement balance handling responsiveness against stability risks. Low roll centers, often 50–100 mm above ground in passenger cars, promote neutral and better ride isolation by minimizing geometric load transfer, allowing anti-roll bars to fine-tune behavior. However, excessively low positions—below ground level—intensify effects, where lateral forces produce vertical lift or squat components, potentially destabilizing the vehicle under cornering loads and increasing susceptibility to camber loss. Higher roll centers reduce but stiffen the geometric response, leading to abrupt handling transitions and reduced compliance over bumps.

Dynamic Properties

Spring, Wheel, and Roll Rates

In automotive suspension , the spring rate quantifies the stiffness of a suspension spring, defined as the force required to produce a unit deflection in the spring. It is typically expressed in units such as pounds per inch (lb/in) or newtons per millimeter (N/mm). The fundamental equation for spring rate kk is k=Fδk = \frac{F}{\delta}, where FF is the applied force and δ\delta is the resulting deflection. The wheel rate represents the effective stiffness experienced at the wheel , accounting for the mechanical leverage introduced by the suspension's motion ratio, which is the ratio of spring (or damper) travel to vertical wheel travel. This adjustment is crucial because the spring is often not mounted directly above the wheel, altering the force transmission. The wheel rate is calculated as wheel rate=k×(motion ratio)2\text{wheel rate} = k \times (\text{motion ratio})^2, where kk is the spring rate; the squaring arises from the combined effect of force amplification and displacement reduction in the linkage geometry. Roll rate, also known as roll stiffness, measures the suspension's resistance to body roll during cornering, primarily provided by the springs and anti-roll bars, and is expressed in units like newton-meters per degree (Nm/°). For a given , it can be approximated by considering the geometric configuration, with the equation roll rate=k×t22\text{roll rate} = \frac{k \times t^2}{2}, where kk is the wheel rate and tt is the track width; this formulation accounts for the torsional resistance generated by the differential deflection of the springs across the axle. The roll couple percentage describes the distribution of total roll stiffness between the front and rear axles, typically expressed as the front axle's contribution to the overall roll resistance (e.g., 50% for neutral balance). This percentage is tuned to influence vehicle handling balance: a higher front percentage promotes understeer by directing more lateral load transfer forward, while a lower front percentage encourages oversteer by shifting it rearward. These rates collectively govern vertical compliance and lateral stability, with their interplay affecting weight transfer during maneuvers such as cornering.

Weight Transfer and Jacking Effects

Weight transfer in automotive suspensions refers to the redistribution of vertical loads on the wheels during dynamic maneuvers such as cornering, where lateral causes a shift from the inside to the outside wheels. This phenomenon is fundamental to handling, as it directly influences grip and stability. In corners, the total lateral weight transfer combines contributions from both sprung and unsprung masses, with the sprung portion dominating due to its greater magnitude. Sprung weight transfer occurs as the vehicle's body (sprung mass) rolls under the influence of centrifugal force, creating a moment about the roll axis that alters wheel loads. The magnitude of this lateral transfer for the sprung mass is given by the equation: ΔWs=msayhst\Delta W_s = \frac{m_s \cdot a_y \cdot h_s}{t} where msm_s is the sprung mass, aya_y is the lateral acceleration, hsh_s is the height of the sprung mass center of gravity above the roll axis, and tt is the track width. This transfer increases the load on the outside wheels while reducing it on the inside, potentially limiting overall cornering grip if excessive. Unsprung weight transfer, in contrast, results from direct inertial forces acting on components like wheels, tires, and suspension arms that are not isolated by springs. Since the unsprung mass center of gravity is low and close to the ground, its transfer is smaller but acts without the filtering effect of the suspension, directly affecting wheel vertical loads. The formula for unsprung lateral transfer is similar in form: ΔWu=muayhut\Delta W_u = \frac{m_u \cdot a_y \cdot h_u}{t} where mum_u is the unsprung mass and huh_u is its center of gravity height, typically near tire radius. This direct loading can amplify road irregularities' impact on traction during cornering. Jacking effects stem from misalignment between the and the vehicle's overall geometry, where lateral forces at the contact patch produce a vertical component that lifts or squats the . This upward lift, known as , occurs when the roll center is elevated, creating a for the lateral . The jacking can be approximated as: Fj=FyhrcLF_j = F_y \cdot \frac{h_{rc}}{L} where FyF_y is the lateral , hrch_{rc} is the roll center height, and LL is the wheelbase; this approximation holds for small geometric angles. Such forces raise the vehicle body, altering suspension geometry and load distribution. In high-performance vehicles, excessive reduces stability by unloading the inside wheels further, diminishing traction and increasing the risk of oversteer or rollover under high lateral loads. This effect is particularly pronounced in setups with high roll centers, where the vertical lift compromises tire consistency and overall handling predictability.

Components and Mechanisms

Springs

Springs in passive car suspensions serve as the primary elements for storing and releasing to absorb road irregularities and maintain vehicle stability. They support the vehicle's weight while allowing controlled vertical movement of the wheels, contributing to ride comfort and handling. Common types include coil, , torsion bar, and air springs, each suited to specific applications based on their mechanical properties and design. Coil springs, typically helical in shape, are widely used in independent suspension systems for their ability to provide a smooth ride by compressing and extending linearly or progressively. Made primarily from high-carbon alloys, they offer good ride comfort due to their consistent deflection under load, making them ideal for passenger cars where isolation from road harshness is prioritized. Progressive-rate coil springs feature variable coil spacing or wire thickness to increase as compression increases, providing softer initial response for comfort and firmer support during cornering; linear-rate versions maintain constant throughout . Pros include versatility in design and superior comfort over rough surfaces, while cons encompass limited load-bearing capacity compared to other types and potential for coil bind at full compression, which can restrict wheel . and durability are enhanced in modern designs through and shot-peening to resist cracking under cyclic loading. Leaf springs consist of multiple layered steel strips, often parabolic in shape, that act as both springs and locating links in solid axle setups, particularly for trucks and rear suspensions. Constructed from high-strength alloy steels like 5160 or 1095, they excel in load-bearing applications by distributing weight evenly across the layers, offering superior durability for heavy-duty use and inherent damping from inter-leaf friction. Pros include high strength for towing and hauling, low cost, and simplicity in maintenance, while cons involve a harsher ride due to progressive stiffening and limited articulation, which can reduce off-road performance. Durability is a key strength, with resistance to fatigue from their multi-layer design, though corrosion in harsh environments can accelerate wear; modern tapered or multi-leaf configurations mitigate this by reducing weight and stress concentrations. Torsion bar springs employ a straight or slightly curved metal bar that twists about its longitudinal axis to provide spring action, commonly installed in front suspensions of trucks and SUVs. Typically made from heat-treated , they function by resisting torsional deformation, allowing for adjustable via an arm and adjustment bolt. Pros encompass compactness, which saves underbody space, and ease of height tuning without replacing components, while cons include linear rate characteristics that limit progressive response and potential for binding in extreme travel. Installation often orients the bar longitudinally along the , with one end anchored to the frame and the other connected to a , facilitating transverse load handling in systems. Fatigue resistance is achieved through alloy selection and surface treatments, though they are prone to stress concentrations at points over time. Air springs utilize pressurized air within rubber or bladders to support the , often integrated with independent or air-ride systems for adjustable height and load leveling. Constructed from reinforced rubber composites with internal guides, they provide a near-linear rate that can be tuned via air pressure for varying payloads. Pros include exceptional ride comfort through isolation of vibrations and automatic leveling for consistent handling, while cons involve higher complexity, susceptibility to leaks, and elevated maintenance costs due to and requirements. Durability depends on bellow material quality, with modern designs using fiber-reinforced rubber to withstand up to 1 million cycles before fatigue sets in. Spring materials have evolved from traditional high-carbon steels, valued for their high yield strength and resistance, to advanced composites like carbon fiber-reinforced polymers in hybrid designs for select applications. Composite springs, for instance, reduce weight by up to 70% compared to equivalents while maintaining equivalent , improving and ride quality through better properties. This shift addresses limitations in steel's weight and issues, with composites offering superior life in non-corrosive environments, though they remain costlier and less common in mass-market vehicles. Progressive versus linear rates are selected based on application needs, with the former preferred for balanced comfort and control; detailed rate calculations are covered in dynamic properties analysis. Installation orientations vary: longitudinal setups, common for and torsion bars in axles, align springs parallel to the vehicle's direction for direct load path, while transverse orientations, used in some coil or front suspensions, span side-to-side for enhanced roll stability in compact .

Dampers and Shock Absorbers

Dampers, commonly known as shock absorbers, function primarily to provide viscous in automotive suspensions by resisting the relative motion between the sprung and unsprung masses through resistance. This process converts from suspension oscillations into via fluid shear and orifice flow, thereby controlling vertical motion and preventing excessive bouncing after encountering road irregularities. In conjunction with springs, which store and release energy based on position, dampers offer velocity-dependent resistance to maintain stability and comfort. The force generated by shock absorbers is typically tuned differently for compression (jounce) and (extension) phases to optimize ride quality and handling. During compression, lower allows the suspension to absorb impacts more compliantly, while higher prevents the wheel from rapidly extending after a bump, reducing body roll and improving contact with the road. This asymmetry in valving—achieved through orifices and shims—ensures that the suspension returns to equilibrium efficiently without overextending. Common types of hydraulic shock absorbers include twin-tube and monotube designs, both of which rely on viscous for but differ in and . Twin-tube absorbers feature an inner tube containing the and , surrounded by an outer reserve tube that accommodates displaced during operation; this is cost-effective and suitable for everyday vehicles but can suffer from under high loads. Monotube gas-charged absorbers, in contrast, use a single high- divided by a floating separating the hydraulic from a nitrogen gas charge, which prevents and foaming for more consistent , particularly in applications. The gas charge in both types maintains to enhance responsiveness, with monotubes often preferred for their superior heat dissipation and fade resistance during . Adjustable valving in shock absorbers allows for manual or mechanical tuning of characteristics, typically through external knobs or reservoirs that alter orifice sizes or shim stacks for compression and independently. Single-adjustable units often focus on , while double- or triple-adjustable variants provide finer control over low- and high-speed , enabling customization for specific conditions or track setups. These features extend to integration with electronic controls in advanced passive systems, where valves modulate fluid flow based on inputs for real-time adjustments without fully active intervention. The effectiveness of damping is quantified by the damping ratio ζ\zeta, a dimensionless measure of how quickly oscillations decay relative to critical damping: ζ=c2km\zeta = \frac{c}{2 \sqrt{k m}}
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