To find the gravitational force on a fourth particle \( P \) when placed at a distance of \( 13 \, \text{m} \) from the particle \( B \) on the perpendicular bisector of the line \( AC \), we'll follow these steps using Newton's law of universal gravitation.
- According to Newton's law of gravitation, the gravitational force between two masses \( m_1 \) and \( m_2 \) is given by: \(F = \frac{G \cdot m_1 \cdot m_2}{r^2}\) where \( G \) is the gravitational constant and \( r \) is the distance between the masses.
- Consider particles \( A, B, \) and \( C \) aligned in a straight line with \( AB = BC = 13 \, \text{m} \). The fourth particle \( P \) is placed at a distance of \( 13 \, \text{m} \) from particle \( B \) on the perpendicular bisector of the line \( AC \). Thus, \( P \) is also equidistant from \( A \) and \( C \).
- Assuming \( M = 100 \, \text{kg} \) for each particle \( A, B, C, \) and \( P \), we find \( P \) is positioned on the perpendicular bisector forming a right triangle with \( AB \) and \( BC \). The distances \( PA = PC = \sqrt{13^2 + 6.5^2} = \sqrt{169 + 42.25} = \sqrt{211.25} \approx 14.53 \, \text{m}\).
- The force due to \( B \): \(F_B = \frac{G \cdot M \cdot M}{13^2} = \frac{G \cdot 100 \cdot 100}{169} = \frac{10000G}{169} \approx 59.17G\)
- The force on \( P \) due to \( A \) and \( C \) (which are equidistant) add up vectorially. Since they are symmetrically placed and \( PA = PC \): \(F_{A} = F_{C} = \frac{G \cdot 100 \cdot 100}{(14.53)^2} \approx \frac{10000G}{211.25} \approx 47.34G\) The horizontal components cancel, and the vertical components add up: \(F_{\text{net}, AC} = 2 \cdot F_A \cdot \frac{6.5}{14.53} \approx 2 \times 47.34G \times 0.447 \approx 42.34G\)
- Total gravitational force \( F \): \(F_{\text{total}} = F_B + F_{\text{net}, AC} \approx 59.17G + 42.34G = 101.51G \approx 100G\)
Thus, the gravitational force on the particle \( P \) is approximately 100 G.