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A similar conclusion can be obtained with the triangle AOB at the. 4.1, which proves the point O AO and BO is at the center of the perpendicular RADIUS arc trajectory. If the angle α is constant, then save both path and becomes a concentric-circle s1 with RADIUS R and R/tan α. In this way, using equation (4.14), you can rewrite the equation of motion (4.8) in the following form:
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