Drive Shafts |
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General fundamental theory | ||
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Kinematics of Hooke's joints
1. The joints In the theory of mechanics the cardan joint or Hooke's joint is defined as a spatial or spherical drive unit with a non-uni form gear ratio or transmission. The transmission behaviour of this joint is described by the equation. |
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In this equation ![]() ![]() ![]() |
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A measure for the non-uniformity is the
difference of the rotation angles
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Expressed by an equation, that means:
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![]() ![]() (also called gimbal error) ![]() b) Gear ratio ![]() |
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The following diagram shows the gear ratio i = ![]() ![]() |
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The degree of non-uniformity U is
defined by: U = i max. - i min. = tan β * sin β where: ![]() |
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The diagram shows the course of the
degree of nonuniformity U and of the angular difference
![]() From the motion equation it is evident that a homokinematic motion behaviour corresponding to the dotted line under 45° - as shown in the diagram - can only be obtained for the deflection angle β = 0°. A synchronous or homokinematic running can be achieved by a suitable combination or connection of two or more joints. |
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2. The universal shaft The rotation angle difference ![]() 1) The deflection angles of both joints must be equal, i.e. ![]() Two arrangements are possible: |
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2) The two joints must have a kinematic
angular relationship of 90° (![]() For a more intensive study of universal shaft kinematics we refer you to the VDI-recommendation 2722 to the relevant technical literature. |
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