C368/88 © IMechE 1988
The development of a differential for the improvement
of traction control
S E CHOCHOLEK, BSME
Gleason Corporation, Rochester, New York, United States of America
SYNOPSIS: An introduction to the function of Gleason's TORSEN differential including discussions of its major characteristics, design flexibilities, and effects on vehicle performance.
1 INTRODUCTION
Traction management ... the ability to match available power to actual road conditions ... is a concern shared by drivers and automotive engineers alike. With the Torsen differential, Gleason is meeting this challenge of improving traction management in both front and rear wheel drive vehicles, all-wheel drive vehicles, and in a variety of applications of the various drives for use in cars, trucks, military vehicles, construction and utility vehicles, and racing cars.
This paper explains the basic operating functions, various design alternatives, and the possibilities for improving traction management provided by the Torsen differential.
2 CHARACTERISTIC FUNCTIONS
The Torsen differential provides for the selection of an optimal compromise between the two primary functions of any differential, namely, transmitting power from a single power source to two drive axles (or shafts) and permitting independent rotation of the two driven axles (i.e., differentiation). This compromise enables an increase in the total amount of torque which can be conveyed by the drive axles under all traction conditions, without unduly restricting differentiation. Differentiation is necessary to accommodate different rotational speeds between drive axles due to vehicle turning situations and variations in tire rolling radii. These objectives are accomplished by associating the function of differentiation with a proportioning torque between drive axles. The significance of this important characteristic will be apparent from the following discussion, beginning with an explanation of torque transfers within a differential.
2.1 A general statement of differential torque transfers
One of the two above-mentioned primary differential functions, the transmission
of power from a
single driveshaft to the two driven axles is most closely associated with
the objective of traction
management (see Figure 1). Power, of course, is the product of torque and
rotational speed.
However, since it is possible to express vehicular traction as a reaction
force acting at a given drive wheel radius, traction considerations related
to the function of power transfer to the drive axles may be expressed in
terms of torque alone.
Actually, two types of torque transfers may be 2.2 Comparison with open differential The just-mentioned characteristic of the |
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It is this type of problem which is most often identified with the need
for improved traction
management (see Figure 2). The Torsen differential addresses this need by
providing for a torque
proportioning characteristic between drive axles by interconnecting the
drive axles with an Invex
gearing arrangement. This gearing is designed to support a predetermined
ratio of torques between drive axles.
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2.3 Invex gearing Invex gearing in a Torsen differential includes a gear train arrangement
comprised of two or more pairs of satellite gears (called element |
The modified crossed axis helical gear mesh, element gear to side gear, is designed and processed to provide instantaneous elliptical contact for reduced tooth stress and increased tooth overlap engagement. In addition, gear tooth helix angle, pressure angle and tooth depth proportions are selected to further minimize stress and wear without sacrifice to function.
2.4 Torque bias ratio
The maximum torque ratio which is supported by a particular differential design is termed 'bias ratio'. This term is expressed as the quotient of the torque in the higher torque axle divided by the torque in the lower torque axle in proportion to unity.
The provision of bias ratio significantly affects the operative connection
between drive axles and
represents a careful choice for controlling torque transfers between drive
axles to achieve optimum traction. A '4:1' bias ratio design means that
the Torsen differential is capable of delivering, to the drive wheel having
better traction, four times the amount of torque which can be supported
by the lower traction drive wheel. In comparison with an open differential,
this means that, under the same conditions, a '4:1' bias ratio differential
is capable of delivering approximately two and one-half times more torque
to the drive axles collectively than an open differential.
2.5 Comparison with other types of differentials
Other means are also known for modifying the operative connection between drive axles to provide for the transfer of additional torque to the drive axles collectively. For example, many limited-slip differentials provide for preloading friction clutches to oppose the transfer of torque between drive axles. This frictional pre-load represents a particular minimum magnitude of resistance which must be overcome to permit any relative rotation between drive axles which may interfere with the operation of anti-lock braking systems. Also, since frictional forces are continually active to resist differentiation, the friction clutches tend to wear, resulting in a deterioration of intended differential performance.
In contrast to the limited-slip's continuous magnitude of frictional
resistance to differentiation, the
torque biasing characteristic of the Torsen differential provides for a
maximum ratio of torque
distributions between drive axles. For instance, as the amount of torque
being conveyed by the
Torsen differential decreases, the amount of resistance to differentiation
also decreases. That is, even though the bias ratio remains relatively constant,
a proportional division of a lower magnitude of torque being conveyed by
the differential results in a smaller torque difference between drive axles.
In braking situations where little or no torque is being conveyed by the
differential, a four to one apportionment of torque between drive axles
amounts to little or no torque difference between drive axles. Thus, the
Torsen differential will not support any appreciable torque 'wind-up' between
drive axles during braking and so does not interfere with the operation
of anti-lock braking systems.
Another known approach to modifying the operative connection between drive axles is to provide for resisting differentiation as a function of the speed difference between drive axles. It has long been appreciated that undesirable wheel slip is associated with very high rates of differentiation. Differentials have been designed using fluid shear friction, which respond to increased rates of differentiation by increasing fluid shear frictional resistance to differentiation. The obvious problem with such 'speed sensitive' differentials is that undesirable wheel slip has already occurred well in advance of its detection. Also, the fluid shear friction designs generally rely on the changes in fluid temperature associated with high differential shear rates to increase resistance to differentiation. However, similar temperature changes may be associated with extended periods of desirable differentiation, or may be influenced by changes in ambient temperature, so that resistance to differentiation may vary throughout ordinary conditions of vehicle use.
The bias ratio characteristic of the Torsen differential instantly reacts to unequal traction conditions by delivering an increased amount of torque to the drive wheel having better traction before the other drive wheel exceeds the limit of traction available to that wheel. The bias ratio characteristic also remains substantially constant over a wide range of torque conveyed by the differential, and is not sensitive to changes in ambient temperature or conditions of vehicle use.
3 STRUCTURE FOR ACHIEVING TORQUE BIAS
As previously stated, the torque biasing characteristic of the Torsen
differential is achieved by
interconnecting the drive axles with an Invex gearing configuration which
selectively controls the
generation of frictional torques within the differential. It is important
to note that there are no intrinsic forces or pre-loads within the differentials
which affect transfers of torque between drive axles. All of the forces
which are controlled to produce frictional resistance between drive axles
are derived from transfers of torque between a single drive source and the
drive axles.
The characteristic of torque bias is achieved in a very simple way. It
is well known that frictional
forces are determined by the product of the coefficient of friction of a
given surface and the normal force applied to that surface. Frictional torque,
of course, is merely the application of that normal force at an effective
frictional radius. All of the forces which are active within the differential
are derivable from the torque which is being conveyed by the differential
and the friction coefficients of surfaces within the differential. Therefore,
all of the frictional forces which are generated within the differential,
and all of the resulting resistant torques which oppose the transfer of
torque between drive axles, are proportional to the torque being conveyed
by the differential. Since the maximum difference in torque between drive
axles which can be supported by friction is proportional to the combined
torque of the drive axles, the maximum bias ratio remains constant with
respect to changes in the combined drive axle torques.
In addition to providing a geared interconnection between drive axles
which permits the usual
opposite relative rotation between the drive axles, the gearing also distributes
forces which may be generated to resist differentiation over a large number
of different surfaces within the differential. The surfaces over which the
Invex gearing distributes forces are designed with different coefficients
of friction and the Invex gearing is designed to distribute different loads
between the surfaces. Collectively, the surfaces and the gearing are designed
to distribute wear evenly over the surfaces and to control the overall amount
of friction within the differential needed to achieve a desired bias ratio.
3.1 Major components of the Torsen differential
The twenty-one components which make up the differential are shown in Figure 4 (not included ...didn't reproduce well). All components of the Invex gear system are contained within the housing. Input power usually is transmitted to the housing by way of a ring gear (crown wheel) bolted to the housing itself. Trunnions are adapted to receive bearings by which the housing is rotatively supported and retained within the axle carrier assembly. These trunnions also receive the respective axle ends which are splined to the side gears within the housing.
Each side gear meshes with element gears arranged at intervals about the periphery of the associated side gears; tangent to, and in engagement with, the pitch surfaces of the side gears. Each of these element gears is formed with a helical middle portion and spur gear end portion. Each side gear meshes with the middle portion of these associated element gears. At the same time, the integral spur gear portion of each element gear meshes with the spur portion of its adjacent element gear. Element gears are shaft-mounted by means of their associated journal pins. The number of element gears and associated hardware may vary. However, the usual arrangement has three sets of element gear pairs arranged at 120 degree intervals as illustrated by Figure 3. It is this arrangement of Invex gearing that provides for (a) connecting the drive axles for opposite directions of relative rotation with respect to the differential housing and, (b) controlling the transfer of torque between drive axles.
Completing the hardware complement are thrust washers used between each end of each side gear, between side gears and the housing. Selection of thrust washers is important in determining the operating characteristics for each application. Proprietary Gleason models permit preselection of components with a high degree of accuracy with respect to actual vehicle characteristics.
3.2 A mathematical representation of the Torsen differential
This section of the paper provides a mathematical representation of the basic frictional relationships within a Torsen differential which are responsible for achieving the bias characteristic between drive axles. The mathematical representation assumes that the direction of torque transfer through the differential is from a vehicle's engine to the drive axles. Figure 4 may be again referred to for identifying differential components mentioned in this section. However, specific forces and torques which are mentioned in this section are illustrated in Figure 5 in association with a schematic depiction of key differential components.
Engine torque applied to the ring gear (Trg) is substantially equal in magnitude to the sum of reaction torques which are developed at each drive axle (T1, T2). The engine torque is transferred to the drive axles through (a) the differential housing which supports the ring gear and |
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(b) the Invex gearing which is carried within the housing and interconnects the drive axles for equal but opposite directions of relative rotation with respect to the housing.
Thus, in addition to transferring torque from the differential housing
to the drive axles, the Invex
gearing also provides a rotational interconnection between drive axles which
may be understood to function as a gear train for transferring torque between
drive axles. Gear trains, of course, develop various reactions at gear meshes
and mounting surfaces which generate friction opposing rotation of the train
in proportion to the torque being carried by the train. Since all of the
engine torque which is transferred to the drive axles is carried by the
Invex gearing, reaction torque which opposes rotation of the Invex gearing
is proportional to the engine torque which is transferred to the drive wheels.
Thus, the transfer of torque between drive axles is also resisted in proportion
to the transfer of torque between the engine and drive axles.
This feature enables the Torsen differential to support a torque imbalance between drive axles which contributes to the total amount of torque which can he transferred from the engine to the drive axles when the amount of torque which can be supported in one of the drive axles is limited by available traction. The major frictional interfaces which are responsible for supporting a torque difference between drive axles are listed below along with parenthetically enclosed symbols representing the coefficients of friction of the respective interfaces.
Side gear to element gear Invex gear meshes (µ1,) Element gear faces to differential housing (µ2) Side gear face to side gear face (µ3) Side gear face to differential housing (µ4) |
Typically, the largest reaction forces within the differential are side
gear thrust forces (Fa1 , Fa2)
resulting from normal tooth loads (F1 , F2) acting at the side gear to element
gear Invex tooth
meshes. The reaction forces are related to the normal tooth loads according
to the following
equation:
Fa1 , Fa2 = (F1 , F2) x Cos ø x Cos ß |
where 'ø' is the tooth normal pressure angle and 'ß' is the side gear helix angle.
These reaction forces are opposed by the respective frictional interfaces
associated with the end
faces of the side gears and result in the generation frictional torques
(Tf3 , Tf4) which oppose side gear rotation. These frictional torques are
related to the reaction forces according to the following equation:
Tf3 , Tf4 = (Fa1 , Fa2) x (R3 , R4) x (µ3 , µ4) |
where 'R3' and 'R4' are the effective friction radii at the respective side gear interfaces.
Frictional torques (Tf5 , Tf6) are developed at the respective interfaces between the element gears and differential housing. These frictional torques are also developed as a result of reaction forces at the side gear to element gear meshes, but the reaction forces being considered here are those which are directed along the respective axes of the element gears. These reaction forces (Fb1 , Fb2) are related to the normal tooth loads according to the following equation:
Fb1 , Fb2 = (F1 , F2) x Cos ø x Cos ß |
The above-mentioned frictional torques (Tf5 , Tf6) are related to the
reaction forces (Fb1 , Fb2)
according to the following equation:
Tf5 , Tf6 = (Fb1 , Fb2) x (R5 , R6) x (µ5 , µ6) |
where 'R5' and 'R6' are the effective friction radii at the respective element gear to housing interfaces.
In addition to the frictional torques developed at the Invex gearing mounting surfaces, sliding contact between the side gears and element gears at the respective Invex gear meshes also produces frictional torques which contribute to supporting a torque division between drive axles. The respective friction forces at the Invex gear meshes may be represented as:
Fc , Fd = (F1 , F2) x (µ1) |
The resulting frictional torques (Tf1 , Tf2) opposed to side gear rotation is related to mesh friction as follows:
Tf1 , Tf2 = (Fc , Fd) x R x Sin ø x Sin ß |
where 'R' is the pitch radius of the respective side gears.
Therefore, the maximum difference torque which can be supported between drive axles is related to each of the above-equated frictional torques as follows:
T1 - T2 = Tf1 + Tf2 + Tf3 + Tf4 + (R / Rc) x (Tf5 + Tf6) |
where 'Rc' is the pitch radius of the combination gears.
Letting the torque difference between drive axles (T1 - T2) be represented by 'Td', it follows that:
T1 = (Trg + Td) / 2, and T2 = (Trg - Td) / 2 |
From this, the maximum ratio of torque which can be supported between drive axles (i.e., bias ratio) is expressed by the following proportion:
torque bias = T1 / T2 : 1 |
An alternative way of referring to drive axle torque distributions is by the term 'percent locking'. This term may be mathematically expressed as follows:
percent locking = (Td / Trg) x 100 |
Figure 6 shows the relationship between torque bias and percent locking over a range of comparable values of each.
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4 DESIGN FLEXIBILTIES The Torsen design provides several options for |
4.1 Overall bias control
The Torsen differential may be designed with different bias ratios ranging
from approximately '2.5:1' to '6:1' or higher. This may be accomplished
by varying the side gear helix angles, or by altering the friction characteristics
for the primary components. An increase in helix angle increases the thrust
component of the side gear meshes along the axis of the side gears so that
smaller portions of the loads communicated by the side gear meshes are related
to rotation of the side gears. In addition, the higher thrust component
along the axis of the side gears increases frictional resistance at the
end faces of the side gears which opposes side gear rotation and thereby
further contributes to an increase in bias ratio.
4.2 Bias ratios between opposite directions of differentiation
The Torsen differential can also be designed so that different bias ratios are associated with different directions of differentiation between drive axles. That is, this design permits one drive axle to support a larger proportion of total drive axle torque than the other. The interaction of forces within the differential which give rise to this design characteristic are very complex. However, it may be generally explained that such different bias ratios are obtained by relatively raising the coefficient of friction which is effective between the end face of one side gear and the differential housing. This tends to increase resistance to the rotation of the drive axle associated with the one side gear with respect to the other drive axle.
This feature may be particularly advantageous in 'center box' applications
where the Torsen
differential is used to interconnect drive shafts to the front and rear
drive axles with a single power source. In this application, it is possible
to set different limits to the maximum proportions of torque which can be
unequally divided between the front and rear drive axles. Since division
of torque is automatically achieved by the Torsen differential in proportion
to available traction, a separate 'torque splitter' is not required. In
fact, such a predetermined torque split may detract from the designed torque
biasing operation.
4.3 Bias ratios between drive and coast modes
It is also an important design freedom to provide for different effective bias ratios between vehicle driving and coasting modes. Since the Torsen differential is designed to have little or no effect on vehicle performance unless torque is being transferred by the differential, it should be understood that what is meant by the coasting mode is actually vehicle deceleration caused by engine braking. This mode is most evident with standard shift vehicles engaged in downshifting.
Invex gearing also makes possible this important design alternative (see
Figure 7). The side gears
within the differential are designed with the same hand of helix angle.
When engine power is applied to the differential (i.e., drive mode), both
side gears are thrust against the same end of the differential housing.
Alternatively, when the engine is used to brake the drive wheels (i.e.,
coast mode), the side gears are thrust against the opposite end of the housing.
This feature provides an opportunity to vary frictional characteristics
between opposite ends of the housing to vary bias ratios between the opposite
directions of power transfer through the differential.
The possibilities for independently varying bias 5 TORSEN DIFFERENTIAL The Torsen design makes important |
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5.1 Vehicle travel on straight roads
On smooth, dry, straight road surfaces, with no apparent traction management
problem, Torsen
differential performance is virtually undetectable from that of an open
differential.
However, on slippery road surfaces where one of the drive wheels does not have adequate traction to support at least one-half of the applied engine torque to the differential housing, the Torsen differential delivers an increased amount of the applied torque to the drive wheel having better traction. The amount of additional torque which can be delivered to the wheel having better traction is limited only by the bias ratio or the amount of traction available to that wheel. Of course, it is never possible to deliver more torque to the drive wheels than the torque which combined traction of the drive wheels will support. However, a Torsen differential designed with an appropriate bias ratio assures that, for most vehicle operating conditions, the vehicle can deliver all of the torque which combined traction of the drive wheels will support.
5.2 Vehicle travel through turns
In turning situations, the outside wheels of a vehicle travel over more distance than the inside wheels. Accordingly, the inside and outside drive wheels must rotate at slightly different speeds (i.e., differentiate) to maintain rolling traction with the road. A torque division between drive axles at the bias ratio is a precondition for differentiation under all circumstances of operation. Essentially, in order for one drive wheel to rotate faster than the other, the drive wheel having greater resistance to rotation slows with respect to the differential case and transfers torque to the other wheel contributing to its faster rotation. The Torsen differential resists transfers of torque between drive wheels in proportion to the torque applied to the differential housing, and this results in a larger proportion of the applied torque being delivered to the slower rotating drive wheel. Therefore, bias ratio should be selected to provide the maximum traction advantage that will still allow both drive wheels to deliver significant portions of engine torque in turns.
However, even in turning situations, the Torsen differential enhances
traction management. Since
torque is already distributed in increased proportion to the inside drive
wheel, it is exceedingly
unlikely that the outside drive wheel will ever exceed available traction
and 'spin up'. Alternatively, should the torque of the inside wheel exceed
available traction in a turn, it is equally unlikely for this wheel to 'spin
up' since such a 'spin up' would still require a difference in traction
between drive wheels which exceeds the bias ratio. Ordinarily, when the
inside wheel exceeds available traction, differentiation ceases and torque
is divided in more even proportion between drive axles determined by the
maximum torque that can be sustained by the inside drive wheel. Thus, in
all directions of travel, the Torsen differential will resist 'spin up'
of either drive wheel by instantly dividing torque between drive axles in
proportions up to the bias ratio to match prevailing traction conditions.
.
6. CENTER BOX APPLICATION
Although the differential has been mostly described with respect to its
use between drive axles, it
should be understood that analogous performance can be expected from use
of the differential as an operative connection between drive shafts to the
front and rear axles. For example, traction
management is enhanced in such 'center box' applications by assuring that
more of the traction of the front and rear drive wheels is available for
use.
7. CONCLUSION
The Torsen differential exhibits a torque biasing characteristic which matches available engine power to changing traction conditions. In particular, Invex gearing provides special design opportunities to match different biasing characteristics with different vehicle applications and conditions of use to best accommodate traction considerations in each instance. Gleason's applied engineering can provide optimal Torsen differential designs to meet a wide variety of traction management requirements.
* Invex is a Gleason trademark applied to Torsen differential components.