평벨트에 작용하는 마찰력

Belt tension differs due to friction between the belt and pulley surface. When a pulley rotates counterclockwise, the tension T2 on the side where the belt moves away is greater than T1 on the approaching side. This tension difference enables power transmission and depends on the coefficient of friction and contact angle.

To estimate tensions in a flat belt, you need the total angle of belt-to-surface contact and the coefficient of friction between the belt and pulley. These parameters, combined with force equilibrium analysis, allow you to determine the relationship between tensions at different points along the belt.

A free-body diagram of a differential belt element AB shows forces acting in horizontal and vertical directions. Assuming impending motion, the frictional force opposes belt sliding, causing tension to increase by dT at point B. This differential approach enables integration to find the complete tension relationship across the contact surface.

Friction between the belt and pulley surface determines the maximum tension difference the belt can sustain. At the threshold of impending motion, frictional force reaches its maximum value and directly opposes the belt's sliding motion. This critical condition allows engineers to calculate the tension limits before slipping occurs.

Horizontal and vertical force equilibrium equations applied to a differential belt element yield two relationships. Using cosine and sine approximations, these equations combine to produce an integrated expression correlating belt tensions. This mathematical framework applies to flat belts on any curved contacting surface.

Over-tensioning causes premature wear and reduces system efficiency, while under-tensioning causes belt slippage and reduces power transmission capability. Proper tensioning is achieved by adjusting pulley distance or using a tensioning device to balance performance and durability in belt-driven systems effectively.

In vertical equilibrium equations, the product of two differentials (dT and dθ) is much smaller than first-order differentials and is therefore neglected. This simplification is valid because differential elements are infinitesimally small, making higher-order terms negligible compared to linear terms in mathematical analysis.