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en/6.1.9.md
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| + | ### Statement | ||
| + | |||
| + | $6.1.9.$ [Insert the problem statement] | ||
| + | |||
| + | ### Solution | ||
| + | |||
| + | ### Statement | ||
| + | |||
| + | $6.1.9.$ Two identically charged balls of mass $m$, suspended from the same point on threads of length $\ell$, moved apart so that the angle between the threads became a right angle. Determine the charge of the balls. | ||
| + | |||
| + | <div align="center"> | ||
| + | <img src="https://savchenkosolutions.com/6/6.1.9/statement.png" alt="For problem 6.1.9"> | ||
| + | </div> | ||
| + | |||
| + | ### Solution | ||
| + | |||
| + | In this case, 3 forces act on each ball: the tension force $\vec{T}$, directed along the thread (at an angle of $45^\circ$ to the horizontal); the gravity force $m\vec{g}$; and the Coulomb force $\vec{F}_k$. | ||
| + | |||
| + | Let us write Newton's second law in projections onto the horizontal and vertical axes: | ||
| + | $$Ox: F_k - T \cdot \cos 45^\circ = 0 \quad (1)$$ | ||
| + | $$Oy: T \cdot \sin 45^\circ - mg = 0 \quad (2)$$ | ||
| + | |||
| + | From this, the equalities for the gravity force $m\vec{g}$ and the Coulomb force $\vec{F}_k$ follow: | ||
| + | $$F_k = T \cdot \cos 45^\circ \quad (3)$$ | ||
| + | $$mg = T \cdot \sin 45^\circ \quad (4)$$ | ||
| + | |||
| + | Dividing one equation by the other, we obtain: | ||
| + | $$\frac{F_k}{mg} = \cot 45^\circ = 1 \quad (5)$$ | ||
| + | |||
| + | This equality can be rewritten in the form: | ||
| + | $$\frac{1}{4\pi\varepsilon_0} \frac{q^2}{(\frac{\ell}{\cos 45^\circ})^2} = mg \quad (6)$$ | ||
| + | |||
| + | From where we express the charge of the balls: | ||
| + | $$q = \sqrt{4\pi\varepsilon_0 mg (\sqrt{2}\ell)^2} \implies q = \ell\sqrt{8\pi\varepsilon_0 mg} \quad (7)$$ | ||
| + | |||
| + | #### Answer | ||
| + | $$q = \ell\sqrt{8\pi\varepsilon_0 mg}$$ | ||
| + | |||
| + | #### Answer | ||
| + | |||
| + | [Insert a concise answer or boxed result] | ||
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| ### Statement | |||
| $6.1.9.$ [Insert the problem statement] | |||
| ### Solution | |||
| ### Statement | |||
| $6.1.9.$ Two identically charged balls of mass $m$, suspended from the same point on threads of length $\ell$, moved apart so that the angle between the threads became a right angle. Determine the charge of the balls. | |||
| <div align="center"> | |||
| <img src="https://savchenkosolutions.com/6/6.1.9/statement.png" alt="For problem 6.1.9"> | |||
| </div> | |||
| ### Solution | |||
| In this case, 3 forces act on each ball: the tension force $\vec{T}$, directed along the thread (at an angle of $45^\circ$ to the horizontal); the gravity force $m\vec{g}$; and the Coulomb force $\vec{F}_k$. | |||
| Let us write Newton's second law in projections onto the horizontal and vertical axes: | |||
| $$Ox: F_k - T \cdot \cos 45^\circ = 0 \quad (1)$$ | |||
| $$Oy: T \cdot \sin 45^\circ - mg = 0 \quad (2)$$ | |||
| From this, the equalities for the gravity force $m\vec{g}$ and the Coulomb force $\vec{F}_k$ follow: | |||
| $$F_k = T \cdot \cos 45^\circ \quad (3)$$ | |||
| $$mg = T \cdot \sin 45^\circ \quad (4)$$ | |||
| Dividing one equation by the other, we obtain: | |||
| $$\frac{F_k}{mg} = \cot 45^\circ = 1 \quad (5)$$ | |||
| This equality can be rewritten in the form: | |||
| $$\frac{1}{4\pi\varepsilon_0} \frac{q^2}{(\frac{\ell}{\cos 45^\circ})^2} = mg \quad (6)$$ | |||
| From where we express the charge of the balls: | |||
| $$q = \sqrt{4\pi\varepsilon_0 mg (\sqrt{2}\ell)^2} \implies q = \ell\sqrt{8\pi\varepsilon_0 mg} \quad (7)$$ | |||
| #### Answer | |||
| $$q = \ell\sqrt{8\pi\varepsilon_0 mg}$$ | |||
| #### Answer | |||
| [Insert a concise answer or boxed result] | |||