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Consider an attractive force which is ce...

Consider an attractive force which is central but is inversely proportional to the first power of distance. If a particle is in circular orbit, under such a force , which of the following statements are correct ?

A

the speed is directly proportional to the square root of orbital radius

B

the speed isindependent of radius

C

the period is independent of radius

D

the period is directly proportional to radius.

Text Solution

AI Generated Solution

The correct Answer is:
To solve the problem, we need to analyze the given attractive force, which is inversely proportional to the first power of distance. Let's denote this force as \( F \). According to the problem, we can express this force as: \[ F = \frac{k}{r} \] where \( k \) is a constant and \( r \) is the distance from the center of the force. ### Step 1: Equate the gravitational force to the centripetal force For a particle in circular motion, the centripetal force required to keep the particle in orbit is given by: \[ F_c = \frac{mv^2}{r} \] where \( m \) is the mass of the particle and \( v \) is its speed. Since the attractive force \( F \) provides the necessary centripetal force, we can set these two forces equal: \[ \frac{k}{r} = \frac{mv^2}{r} \] ### Step 2: Simplify the equation We can cancel \( r \) from both sides of the equation (assuming \( r \neq 0 \)): \[ k = mv^2 \] From this equation, we can solve for the speed \( v \): \[ v^2 = \frac{k}{m} \] Taking the square root gives us: \[ v = \sqrt{\frac{k}{m}} \] ### Step 3: Analyze the speed From the expression for \( v \), we see that the speed \( v \) is independent of the radius \( r \). This means that regardless of how far the particle is from the center, its speed remains constant. ### Step 4: Determine the time period The time period \( T \) of the circular motion can be found using the relationship between speed, distance, and time. The distance traveled in one complete orbit (circumference of the circle) is \( 2\pi r \), so we have: \[ T = \frac{\text{Distance}}{\text{Speed}} = \frac{2\pi r}{v} \] Substituting the expression for \( v \): \[ T = \frac{2\pi r}{\sqrt{\frac{k}{m}}} = 2\pi r \sqrt{\frac{m}{k}} \] ### Step 5: Analyze the time period From the expression for \( T \), we can see that the time period \( T \) is directly proportional to the radius \( r \). This means that as the radius increases, the time period also increases. ### Conclusion Based on our analysis, we can summarize the findings: 1. The speed \( v \) is independent of the radius \( r \). 2. The time period \( T \) is directly proportional to the radius \( r \). Thus, the correct statements are: - Speed is independent of the radius (Option 2 is correct). - Time period is directly proportional to the radius (Option 4 is correct). ### Final Answer The correct options are 2 and 4.

To solve the problem, we need to analyze the given attractive force, which is inversely proportional to the first power of distance. Let's denote this force as \( F \). According to the problem, we can express this force as: \[ F = \frac{k}{r} \] where \( k \) is a constant and \( r \) is the distance from the center of the force. ...
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