Gear mechanism that allows driven shafts to spin at different speeds
This block represents a gear mechanism that allows the driven shafts to spin at different speeds. Differentials are common in automobiles, where they enable the various wheels to spin at different speeds while cornering. Ports S, D1, and D2 represent the driving and driven shafts of the differential. Any of the shafts can drive the remaining two.
The block models the differential mechanism as a structural component based on Simple Gear and Sun-Planet Bevel Simscape™ Driveline™ blocks. The figure shows the block diagram of this structural component.
To increase the fidelity of the gear model, you can specify properties such as gear inertia, meshing losses, and viscous losses. By default, gear inertia and viscous losses are assumed negligible. The block enables you to specify the inertias of the gear carrier and internal planet gears only. To model the inertias of the outer gears, connect Simscape Inertia blocks to ports D, S1, and S2.
You can model the effects of heat flow and temperature change through an optional thermal conserving port. By default, the thermal port is hidden. To expose the thermal port, right-click the block in your model and, from the context menu, select Simscape > Block choices. Specify the associated thermal parameters for the component.
Select the placement of the bevel crown gear with respect to
the center-line of the gear assembly. The default is
right of the center-line.
Fixed ratio gD of
the carrier gear to the longitudinal driveshaft gear. The default
Parameters for meshing losses vary with the block variant chosen—one with a thermal port for thermal modeling and one without it.
Vector of viscous friction coefficients [μS μD]
for the sun-carrier and longitudinal driveshaft-casing gear motions,
respectively. The default is
From the drop-down list, choose units. The default is newton-meters/(radians/second)
Moment of inertia of the planet gear carrier. This value must
be positive or zero. Enter
0 to ignore carrier
inertia. The default value is
Moment of inertia of the combined planet gears. This value must
be positive or zero. Enter
0 to ignore gear inertia.
The default value is
Thermal energy required to change the component temperature
by a single degree. The greater the thermal mass, the more resistant
the component is to temperature change. The default value is
Component temperature at the start of simulation. The initial
temperature alters the component efficiency according to an efficiency
vector that you specify, affecting the starting meshing or friction
losses. The default value is
Differential imposes one kinematic constraint on the three connected axes:
ωD = ±(1/2)gD(ωS1 + ωS2) ,
with the upper (+) or lower (–) sign valid for the differential crown to the right or left, respectively, of the center line. The three degrees of freedom reduce to two independent degrees of freedom. The gear pairs are (1,2) = (S,S) and (C,D). C is the carrier.
The sum of the lateral motions is the transformed longitudinal motion. The difference of side motions ωS1 – ωS2 is independent of the longitudinal motion. The general motion of the lateral shafts is a superposition of these two independent degrees of freedom, which have this physical significance:
One degree of freedom (longitudinal) is equivalent to the two lateral shafts rotating at the same angular velocity (ωS1 = ωS2) and at a fixed ratio with respect to the longitudinal shaft.
The other degree of freedom (differential) is equivalent to keeping the longitudinal shaft locked (ωD = 0) while the lateral shafts rotate with respect to each other in opposite directions (ωS1 = –ωS2).
The torques along the lateral axes, τS1 and τS2, are constrained to the longitudinal torque τD in such a way that the power flows into and out of the gear, less any power loss Ploss, sum to zero:
ωS1τS1 + ωS2τS2 + ωDτD – Ploss= 0 .
When the kinematic and power constraints are combined, the ideal case yields:
gDτD = 2(ωS1τS1 + ωS2τS2) / (ωS1 + ωS2) .
In the nonideal case, τloss ≠ 0. See Model Gears with Losses.
Gears are assumed rigid.
Coulomb friction slows down simulation. See Adjust Model Fidelity.
|D||Rotational conserving port representing the longitudinal driveshaft|
|S1||Rotational conserving port representing one of the sun gears|
|S2||Rotational conserving port representing one of the sun gears|
|H||Thermal conserving port for thermal modeling|