In the case of gear transmission, loads transmitted by gearing are theoretically classified into three types: tangential load (Kt), radial load (Kr) and axial load (em>Ka). Those loads can be calculated dynamically (using equations , em class="textImg"> and , described in section (2)). To determine the actual gear loads, these theoretical loads must be multiplied by coefficients considering vibration and impact during operation (ƒw) (ref. Table 5-6) and the gear coefficient (ƒg) (ref. Table 5-8) considering the finish treatment of gears.

Heavy dutybearing for radial load

Even if radial and axial loads are obtained through general dynamic calculation, the actual load becomes greater than the calculated value due to vibration and impact during operation. In many cases, the load is obtained by multiplying theoretical values by the load coefficient.

Ballbearing for radial load

In the case of belt transmission, the theoretical value of the load affecting the pulley shafts can be determined by obtaining the effective transmission force of the belt. For actual operation, the load is obtained by multiplying this effective transmission force by the load coefficient (ƒw) considering vibration and impact generated during operation, and the belt coefficient (ƒb) considering belt tension. In the case of chain transmission, the load is determined using a coefficient equivalent to the belt coefficient. This equation (5-13) is as follows ;

Bestbearing for radial load

Bearing for radial loadchart

The load distribution affecting bearings can be calculated as follows: first, radial force components are calculated, then, the sum of vectors of the components is obtained in accordance with the load direction. Calculation examples of radial load distribution are described in the following section.

[Notes]1) Codes with subscript 1 and 2 shown in equations are respectively applicable to drive side gears and driven side gears.2) Symbols (+) and (−) denote the following ; Symbols in upper row : clockwise rotation accompanied by right-handed spiral or counterclockwise rotation with left-handed spiral Symbols in lower row : counterclockwise rotation with right-handed spiral or clockwise rotation with left-handed spiral

Bearings shown in Exs. 3 to 5 are affected by components of axial force when these bearings accommodate radial load, and axial load (Ka) which is transferred externally, i.e. from gears. For calculation of the axial load in this case, refer to page Dynamic equivalent load.

Loads affecting bearings includes force exerted by the weight of the object the bearings support, transmission force of devices such as gears and belts, loads generated in equipment during operation etc. Seldom can these kinds of load be determined by simple calculation, because the load is not always constant. In many cases, the load fluctuates, and it is difficult to determine the frequency and magnitude of the fluctuation. Therefore, loads are normally obtained by multiplying theoretical values with various coefficients obtained empirically.