A particle moves in a circular orbit under the action of a central attractive force which is inversely proportional to the distance 'r' . The speed of the particle is
A
proportional to ` r^(2)`
B
Independent of `r`
C
proportional to r
D
proportional to 1/r
Text Solution
AI Generated Solution
The correct Answer is:
To solve the problem, we need to analyze the motion of a particle in a circular orbit under the influence of a central attractive force that is inversely proportional to the distance \( r \).
### Step-by-Step Solution:
1. **Identify the Forces Acting on the Particle:**
The particle is moving in a circular orbit due to a central attractive force. This force can be expressed as:
\[
F = \frac{k}{r}
\]
where \( k \) is a constant.
2. **Use Centripetal Force Equation:**
For an object moving in a circular path, the required centripetal force \( F_c \) is given by:
\[
F_c = \frac{mv^2}{r}
\]
where \( m \) is the mass of the particle and \( v \) is its speed.
3. **Set the Attractive Force Equal to the Centripetal Force:**
Since the attractive force provides the necessary centripetal force, we can set these two forces equal to each other:
\[
\frac{mv^2}{r} = \frac{k}{r}
\]
4. **Simplify the Equation:**
We can multiply both sides by \( r \) (assuming \( r \neq 0 \)):
\[
mv^2 = k
\]
5. **Solve for Speed \( v \):**
Rearranging the equation gives us:
\[
v^2 = \frac{k}{m}
\]
Taking the square root of both sides, we find:
\[
v = \sqrt{\frac{k}{m}}
\]
6. **Conclusion:**
The speed of the particle \( v \) is independent of the radius \( r \) and depends only on the constant \( k \) and the mass \( m \).
### Final Answer:
The speed of the particle is given by:
\[
v = \sqrt{\frac{k}{m}}
\]
To solve the problem, we need to analyze the motion of a particle in a circular orbit under the influence of a central attractive force that is inversely proportional to the distance \( r \).
### Step-by-Step Solution:
1. **Identify the Forces Acting on the Particle:**
The particle is moving in a circular orbit due to a central attractive force. This force can be expressed as:
\[
F = \frac{k}{r}
...
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