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en/1.4.6.md
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| + | ### Statement | ||
| + | |||
| + | $1.4.6.$ [Insert the problem statement] | ||
| + | |||
| + | ### Solution | ||
| + | |||
| + | ### Problem | ||
| + | |||
| + | $1.4.6^*.$ An iceboat is a sailing sled. It can only move along the line in which its runners are pointed. The wind blows with a speed $v$ perpendicular to the direction of the iceboat's motion. The sail makes an angle of $30^\circ$ with the direction of motion. What maximum speed can the iceboat reach under this wind? | ||
| + | |||
| + | ### Solution | ||
| + | |||
| + | At the initial moment, when the iceboat is stationary, the air moves relative to it with a velocity $\vec{v}$. | ||
| + | |||
| + | As the iceboat starts moving and acquires its own velocity $\vec{v}_b$, the relative velocity of the wind changes. According to the velocity addition formula, the relative velocity of the wind is: | ||
| + | $$ \vec{v}_{rel} = \vec{v} - \vec{v}_b $$ | ||
| + | |||
| + | Since the absolute wind velocity $\vec{v}$ is perpendicular to the iceboat's velocity $\vec{v}_b$, these vectors form a right-angled triangle. | ||
| + | |||
| + | The wind will continue to exert pressure on the sail and accelerate the iceboat as long as the relative wind velocity $\vec{v}_{rel}$ pushes against it. The iceboat reaches its maximum speed when the wind stops exerting force on the sail. This condition is met when the relative wind velocity vector $\vec{v}_{rel}$ becomes parallel to the sail. | ||
| + | |||
| + | According to the problem, the sail is set at an angle of $30^\circ$ to the direction of the iceboat's motion. Therefore, in the limiting case, the angle between the vectors $\vec{v}_b$ and $\vec{v}_{rel}$ in our right-angled triangle is exactly $30^\circ$. | ||
| + | |||
| + | From this velocity vector triangle, we can express the relationship: | ||
| + | $$ \tan 30^\circ = \frac{v}{v_b} $$ | ||
| + | |||
| + | Solving for the maximum speed of the iceboat $v_b$: | ||
| + | $$ v_b = \frac{v}{\tan 30^\circ} = v \cot 30^\circ $$ | ||
| + | |||
| + | Since $\cot 30^\circ = \sqrt{3}$, we obtain: | ||
| + | $$ v_b = v\sqrt{3} $$ | ||
| + | |||
| + | #### Answer | ||
| + | |||
| + | $$ v_{max} = v\sqrt{3} $$ | ||
| + | |||
| + | #### Answer | ||
| + | |||
| + | [Insert a concise answer or boxed result] | ||
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| ### Statement | |||
| $1.4.6.$ [Insert the problem statement] | |||
| ### Solution | |||
| ### Problem | |||
| $1.4.6^*.$ An iceboat is a sailing sled. It can only move along the line in which its runners are pointed. The wind blows with a speed $v$ perpendicular to the direction of the iceboat's motion. The sail makes an angle of $30^\circ$ with the direction of motion. What maximum speed can the iceboat reach under this wind? | |||
| ### Solution | |||
| At the initial moment, when the iceboat is stationary, the air moves relative to it with a velocity $\vec{v}$. | |||
| As the iceboat starts moving and acquires its own velocity $\vec{v}_b$, the relative velocity of the wind changes. According to the velocity addition formula, the relative velocity of the wind is: | |||
| $$ \vec{v}_{rel} = \vec{v} - \vec{v}_b $$ | |||
| Since the absolute wind velocity $\vec{v}$ is perpendicular to the iceboat's velocity $\vec{v}_b$, these vectors form a right-angled triangle. | |||
| The wind will continue to exert pressure on the sail and accelerate the iceboat as long as the relative wind velocity $\vec{v}_{rel}$ pushes against it. The iceboat reaches its maximum speed when the wind stops exerting force on the sail. This condition is met when the relative wind velocity vector $\vec{v}_{rel}$ becomes parallel to the sail. | |||
| According to the problem, the sail is set at an angle of $30^\circ$ to the direction of the iceboat's motion. Therefore, in the limiting case, the angle between the vectors $\vec{v}_b$ and $\vec{v}_{rel}$ in our right-angled triangle is exactly $30^\circ$. | |||
| From this velocity vector triangle, we can express the relationship: | |||
| $$ \tan 30^\circ = \frac{v}{v_b} $$ | |||
| Solving for the maximum speed of the iceboat $v_b$: | |||
| $$ v_b = \frac{v}{\tan 30^\circ} = v \cot 30^\circ $$ | |||
| Since $\cot 30^\circ = \sqrt{3}$, we obtain: | |||
| $$ v_b = v\sqrt{3} $$ | |||
| #### Answer | |||
| $$ v_{max} = v\sqrt{3} $$ | |||
| #### Answer | |||
| [Insert a concise answer or boxed result] | |||