Новое решение
en/2.3.16.md
+38 −0
| @@ -0,0 +1,38 @@ | |||
| + | ### Statement | ||
| + | |||
| + | $2.3.16.$ [Insert the problem statement] | ||
| + | |||
| + | ### Solution | ||
| + | |||
| + | ### Statement | ||
| + | |||
| + | $2.3.16.$ A weight suspended on a thread of length $l$ was deflected by a distance $r$ from the equilibrium point and released. What is its maximum velocity? | ||
| + | |||
| + | ### Solution | ||
| + | |||
| + | Let's consider the geometry of the system. Let the maximum deflection angle of the thread be $2\alpha$. The distance $r$ is the chord between the initial deflection point $D$ and the lowest equilibrium point $C$. | ||
| + | The vertical height change $h$ (which corresponds to $BC$ in the diagram) can be expressed in two ways: | ||
| + | $$h = l(1 - \cos 2\alpha) = r \sin\alpha$$ | ||
| + | |||
| + | Using the trigonometric identity $1 - \cos 2\alpha = 2 \sin^2\alpha$, we get: | ||
| + | $$2l \sin^2\alpha = r \sin\alpha$$ | ||
| + | From this, we express the sine of half the deflection angle $\alpha$: | ||
| + | $$\sin\alpha = \frac{r}{2l} \quad \text{(a)}$$ | ||
| + | |||
| + | From the law of conservation of energy, the kinetic energy $E_{\text{kin}}$ will be maximal at the lowest point $C$, where the potential energy is minimal. The maximum kinetic energy equals the initial potential energy: | ||
| + | $$\frac{mv_{\text{max}}^2}{2} = mgh = mgr \sin\alpha$$ | ||
| + | Canceling the mass $m$: | ||
| + | $$\frac{v_{\text{max}}^2}{2} = gr \sin\alpha$$ | ||
| + | |||
| + | Expressing the maximum velocity of the weight: | ||
| + | $$v_{\text{max}} = \sqrt{2gr \sin\alpha} \quad \text{(b)}$$ | ||
| + | |||
| + | Substitute the angle expression from (a) into equation (b): | ||
| + | $$v_{\text{max}} = \sqrt{2g \cdot r \frac{r}{2l}} = r\sqrt{\frac{g}{l}}$$ | ||
| + | |||
| + | #### Answer | ||
| + | $$v_{\text{max}} = r\sqrt{\frac{g}{l}}$$ | ||
| + | |||
| + | #### Answer | ||
| + | |||
| + | [Insert a concise answer or boxed result] | ||
| @@ -0,0 +1,38 @@ | |||
| ### Statement | |||
| $2.3.16.$ [Insert the problem statement] | |||
| ### Solution | |||
| ### Statement | |||
| $2.3.16.$ A weight suspended on a thread of length $l$ was deflected by a distance $r$ from the equilibrium point and released. What is its maximum velocity? | |||
| ### Solution | |||
| Let's consider the geometry of the system. Let the maximum deflection angle of the thread be $2\alpha$. The distance $r$ is the chord between the initial deflection point $D$ and the lowest equilibrium point $C$. | |||
| The vertical height change $h$ (which corresponds to $BC$ in the diagram) can be expressed in two ways: | |||
| $$h = l(1 - \cos 2\alpha) = r \sin\alpha$$ | |||
| Using the trigonometric identity $1 - \cos 2\alpha = 2 \sin^2\alpha$, we get: | |||
| $$2l \sin^2\alpha = r \sin\alpha$$ | |||
| From this, we express the sine of half the deflection angle $\alpha$: | |||
| $$\sin\alpha = \frac{r}{2l} \quad \text{(a)}$$ | |||
| From the law of conservation of energy, the kinetic energy $E_{\text{kin}}$ will be maximal at the lowest point $C$, where the potential energy is minimal. The maximum kinetic energy equals the initial potential energy: | |||
| $$\frac{mv_{\text{max}}^2}{2} = mgh = mgr \sin\alpha$$ | |||
| Canceling the mass $m$: | |||
| $$\frac{v_{\text{max}}^2}{2} = gr \sin\alpha$$ | |||
| Expressing the maximum velocity of the weight: | |||
| $$v_{\text{max}} = \sqrt{2gr \sin\alpha} \quad \text{(b)}$$ | |||
| Substitute the angle expression from (a) into equation (b): | |||
| $$v_{\text{max}} = \sqrt{2g \cdot r \frac{r}{2l}} = r\sqrt{\frac{g}{l}}$$ | |||
| #### Answer | |||
| $$v_{\text{max}} = r\sqrt{\frac{g}{l}}$$ | |||
| #### Answer | |||
| [Insert a concise answer or boxed result] | |||