|
|||||
The following article appeared in the April 2008 issue of Power Transmission Engineering. Torque Arm Design Considerations for Shaft-Mounted Speed ReducersTodd R. Bobak Introduction The SMSR may be “fixed” to the machine using an output flange or, in certain instances, its housing may be bolted directly onto the machine. However, situations exist where direct attachment of the SMSR is either not possible or desirable. In such situations, the SMSR is supported only by the shaft that it is intended to drive. When the SMSR is mounted directly onto a driven shaft with no other external support, it must have a torque arm attached to it. A torque arm is a pivoted, connecting link between the reducer and a fixed anchor point intended to resist the torque developed by the reducer. Quite simply, a torque arm transmits the reaction torque produced by the SMSR into the structure of the machine, thereby preventing the counter-rotation of an SMSR during operation. Most manufacturers of shaft-mounted speed reducers have designed, and offer for purchase, standard torque arms for their products. Situations may exist, however, where a manufacturer’s torque arm does not meet the needs of a certain application (due to space limitations, for example). In such situations, the machine designer may be required to design his or her own torque arm to fit within the constraints of the application. This article provides some design guidelines for such a situation. Resultant Force 1. The torque capacity of the SMSR. As the name implies, this is the mechanical capacity (typically expressed in terms of inch-pounds or Newton-meters) that the SMSR is capable of developing at its output. While it may be tempting to simply multiply the motor output torque by the reducer’s reduction ratio to obtain an output torque value, it is recommended to consider (at a minimum) the larger of the following values: the SMSR’s output torque capacity (as listed in the product catalog) or, the product of the motor’s output torque and reduction ratio times an additional 2.5—to take into account the motor’s starting torque. 2. The dimensional location on the SMSR where the torque arm will be mounted. Manufacturers of shaft-mounted speed reducers provide at least one mounting location for a torque arm (Fig. 1). Note that the point where the torque arm attaches to the reducer (either directly or indirectly through a bracket) is known as the pivot point. Many manufacturers provide more than one potential location for the torque arm in order to accommodate the various mounting configurations available for a given product. The location(s) of these mounting holes/positions may be found in catalog cut sheets or through manufacturer supplied product drawings.
Using Figure 1 as an example, let’s say an application requires a bracket-style torque arm, and this bracket will be attached to the housing at both identified mounting holes. Using the unit model size, reduction ratio, and motor input speed, you can determine the output torque capacity from the reducer catalog ratings table (Fig. 2).
You can also use the catalog dimension sheet to determine the location of the identified mounting holes relative to the center of the reducer’s output bore (Fig. 3).
With this information, you can now calculate the force acting at the selected pivot point, given the fact that torque is the product of force and distance. You can determine the unknown force (F) using these formulas:
It is important to note that during operation, the SMSR will tend to rotate about the driven shaft in the direction opposite to that of the driven shaft’s rotation. With this in mind, it is significant that the calculated force F (above) acts in pure tension on the torque arm. This fact is especially important for torque arms that are long—if they are exposed to compressive forces, they may buckle. Figure 4a shows the correct method of mounting a torque arm so that it is in tension.
Using values from the manufacturer’s specifications (Figures 2 and 3 for our example), you can calculate the resultant force acting at the pivot point as follows:
In essence, the connection method at the pivot point you chose (i.e., bolt, threaded rod, etc.) must be able to withstand this calculated force when in tension. If you find that the calculated force exceeds the physical limits of the connection method, you may choose to incorporate a different, stronger material for the torque arm. A way to minimize this force is to increase the distance L of the pivot point, as shown in Figures 5 and 6. In these examples, the reducer has a T-type torque arm mounted to it, which moves the pivot point an additional 1.85 inches farther from the center of the reducer’s bore.
If all other factors remain the same, this increase in distance yields a decrease of nearly 600 pounds in the force on the torque arm. Thus:
Once again, this calculated force must be compared to the yield stress of the torque arm material to assure that the material limitations are not exceeded. A Turnbuckle for a Torque Arm
You can calculate the force acting at the pivot point in this situation using the same formula for force as in the previous examples. Figures 8-9 show a typical mounting style for a turnbuckle torque arm.
A Note About Mounting Hardware When taking this into account, you must note that the force is not acting on the hardware in tension, but rather in shear. Depending on the location of such hardware, bending movements induced by the force may also be acting on the hardware. Hardware manufacturers usually provide yield and shear limitations for their products. Once again, it is important to compare the calculated forces/stresses acting on the hardware against the published limiting values to assure that the critical points are not exceeded. A Note About Reversing Rotation Recalling that, ideally, a torque arm is mounted so it is in tension, in a reversing application, the torque arm may see a period of time when it also receives compressive forces. Such compressive forces, if great enough, could buckle the torque arm. For such applications, designers may want to add a second torque arm on the opposite side of the SMSR. The second torque arm would take the tension forces generated by the reverse rotation while minimizing the compressive forces on the first torque arm. Angles Other Than 90° In such situations, the designer needs to evaluate the effects of the resultant forces acting on the torque arm. Figure 10 shows a torque arm mounted to an SMSR at some angle (è) that is less than 90°.
Because the torque arm is not acting at a 90° angle to the output bore of the SMSR, there are two forces acting on it. The free-body diagram in Figure 11 details these forces.
The resultant forces (FT and FS) are the component forces of Force “F” acting on the torque arm. These resultant forces place not only a force in tension (FT) acting on the torque arm, but also a shear force (FS). Both forces must be considered when evaluating the strength of the torque arm design. The Effect of Shaft Runout Float may be introduced at the pivot point by attaching rubber bushings to the pivot and anchor points, as shown in Figure 12.
If dual rotation of the output shaft is possible in the application, manufacturers recommend installing rubber bushings on both sides of the pivot and anchor points so float is possible regardless of the direction of rotation. A loose clearance designed between the bolts and through holes in the torque arm bracket may also assist in creating float. In addition to taking precautions to eliminate a rigid mount, designers must also ensure the torque arm is properly aligned when mounting it to the SMSR. Misalignment may inadvertently cause binding that could decrease or entirely eliminate this float. Conclusion Todd R. Bobak has worked in the gear industry for 15 years. He has held positions in technical service, design and development, and quality assurance. He is a product engineer for Sumitomo Drive Technologies in Chesapeake, VA. | ![]() ![]() ![]() ![]() ![]() | ||||