Problem 14
Question
Three particles each of mass \(m\) rotate in a circle of radius \(r\) with uniform angular speed \(\omega\) under their mutual gravitational attraction. If at any instant the points are on the vertex of an equilateral of side \(L\), then angular velocity \(\omega\) is (a) \(\sqrt{\frac{2 G m}{L^{3}}}\) (b) \(\sqrt{\frac{3 G m}{L^{3}}}\) (c) \(\sqrt{\frac{5 G m}{L^{3}}}\) (d) \(\sqrt{\frac{G m}{L^{3}}}\)
Step-by-Step Solution
Verified Answer
Angular velocity \( \omega \) is \( \sqrt{\frac{G m}{L^3}} \), option (d).
1Step 1: Identify Forces Acting on Each Particle
Each particle is subjected to gravitational forces due to the other two particles. Since the particles are at the vertices of an equilateral triangle, we need to consider gravitational force exerted by one point-mass on another.
2Step 2: Calculate Gravitational Force Between Two Particles
The gravitational force between two particles of mass \(m\) at a distance \(L\) is given by Newton's gravitational law: \( F = \frac{G m^2}{L^2} \), where \(G\) is the gravitational constant. This force acts along the side of the equilateral triangle.
3Step 3: Resultant Force Towards Center
For each particle, the resultant force due to the other two particles is directed towards the center of the circle. Since the angle between two gravitational forces is 60°, use the law of cosines for vectors to find the resultant force magnitude as \( F_{ ext{res}} = 2 F imes \cosrac{60°}{2} = F \).
4Step 4: Centripetal Force Requirement
The net gravitational force provides the centripetal force necessary for circular motion. Set the centripetal force required: \( F_c = m r \omega^2 \). The side of the triangle \( L \) satisfies that \( L = 2 imes r \). Include this relationship in the equation.
5Step 5: Express Angular Velocity in Terms of Known Variables
Substitute \( F_{ ext{res}} = F_c \): \( \frac{G m^2}{r^2} = m r \omega^2 \). Simplify to express \( \omega \): \( \omega = \sqrt{\frac{G m}{L^3}} \).
6Step 6: Determine Correct Option
The derived expression for \( \omega \) matches option (d): \( \sqrt{\frac{G m}{L^3}} \). Therefore, the angular velocity \( \omega \) is given by option (d).
Key Concepts
Gravitational ForceCircular MotionCentripetal ForceEquilateral Triangle Geometry
Gravitational Force
Gravitational force is the attractive force that acts between any two masses. It's a fundamental force described by Newton's law of gravitation. According to this law, the gravitational force \( F \) between two masses is calculated using the formula: \[ F = \frac{G m_1 m_2}{r^2} \] where
- \( G \) is the gravitational constant \( 6.674 \times 10^{-11} \, \text{Nm}^2/\text{kg}^2 \)
- \( m_1 \) and \( m_2 \) are the masses of the two objects
- \( r \) is the distance between the centers of the two masses
Circular Motion
Circular motion occurs when an object moves along a circular path. In this exercise, each particle follows circular motion due to both gravitational forces and the resultant force acting towards the center of the circle formed. Characteristics of circular motion include:
- Uniform speed, where the magnitude of the velocity is constant but its direction changes.
- Radius \( r \), the distance from the center of the circle to the particle.
- Angular velocity \( \omega \), the rate of change of the angular position with respect to time.
Centripetal Force
Centripetal force is the inward force required to keep an object moving in a circular path. This force is necessary to constantly change the direction of the object's velocity, ensuring it remains on a curved trajectory rather than moving off tangent.In our scenario, the centripetal force \( F_c \) required for circular motion is \[ F_c = m r \omega^2 \] where
- \( m \) is the mass of the particle
- \( r \) is the radius of the circular path
- \( \omega \) is the angular velocity
Equilateral Triangle Geometry
An equilateral triangle is a triangle where all three sides are of equal length, and all internal angles are 60 degrees. This symmetry is key to simplifying the force analysis in our exercise.When particles are located at the vertices of an equilateral triangle, the geometry allows for specific vector relationships and simplifications:
- Each gravitational force between particles can be easily calculated due to equal side lengths.
- The geometric symmetry helps in determining the resultant forces, using the law of cosines for vectors since each angle is 60 degrees, simplifying to use relationships like \( \cos(60^\circ) = \frac{1}{2} \).
- The distance from the center to any vertex (which is part of determining the circle's radius) can be found using geometric insights.
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