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<h3> Statement </h3>
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$2.1.21.$ The belt lift forms an angle $\alpha$ with the horizon. With what maximum acceleration can a box be lifted on such a lift, if the coefficient of friction is equal to $\mu$? The tape doesn't bend.
<h3>Solution</h3>
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1. By discarding the constraints imposed on the box and replacing them with reactions, we can consider it as a free body capable of moving along the
2. The equation of Newton's second law allows us to determine the maximum value of acceleration
<h4>Answer</h4>
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$$a_{max} = g(\mu\cos\alpha − \sin\alpha )$$
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