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Consider a ring of mass m and radius r. ...

Consider a ring of mass m and radius r. Maximum gravitational intensity on the axis of the ring has value.

A

`(Gm)/(r^(2))`

B

`(2Gm)/(sqrt(3)r^(2))`

C

`(2Gm)/(3sqrt(3)r^(2))`

D

`(Gm)/(2 r^(2))`

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The correct Answer is:
To find the maximum gravitational intensity on the axis of a ring of mass \( m \) and radius \( r \), we will follow these steps: ### Step 1: Understand the Gravitational Intensity Formula The gravitational intensity \( G_P \) at a point \( P \) on the axis of the ring can be expressed as: \[ G_P = \frac{Gm x}{(r^2 + x^2)^{3/2}} \] where: - \( G \) is the gravitational constant, - \( m \) is the mass of the ring, - \( r \) is the radius of the ring, - \( x \) is the distance from the center of the ring to the point \( P \) along the axis. ### Step 2: Differentiate the Gravitational Intensity To find the maximum gravitational intensity, we need to differentiate \( G_P \) with respect to \( x \) and set the derivative equal to zero. Using the quotient rule: \[ \frac{d}{dx} \left( \frac{u}{v} \right) = \frac{v \frac{du}{dx} - u \frac{dv}{dx}}{v^2} \] Let \( u = Gmx \) and \( v = (r^2 + x^2)^{3/2} \). ### Step 3: Apply the Quotient Rule We find: \[ \frac{du}{dx} = Gm \] \[ \frac{dv}{dx} = \frac{3}{2}(r^2 + x^2)^{1/2} \cdot 2x = 3x(r^2 + x^2)^{1/2} \] Now, applying the quotient rule: \[ \frac{dG_P}{dx} = \frac{(r^2 + x^2)^{3/2} \cdot Gm - Gmx \cdot 3x(r^2 + x^2)^{1/2}}{(r^2 + x^2)^3} \] Setting this equal to zero gives: \[ (r^2 + x^2)^{3/2} \cdot Gm - Gmx \cdot 3x(r^2 + x^2)^{1/2} = 0 \] ### Step 4: Simplify the Equation This simplifies to: \[ Gm(r^2 + x^2)^{3/2} = 3Gmx^2(r^2 + x^2)^{1/2} \] Dividing both sides by \( Gm(r^2 + x^2)^{1/2} \) (assuming \( Gm \neq 0 \)): \[ (r^2 + x^2) = 3x^2 \] Rearranging gives: \[ r^2 = 2x^2 \] Thus, we find: \[ x = \frac{r}{\sqrt{2}} \] ### Step 5: Substitute Back to Find Maximum Gravitational Intensity Now substitute \( x = \frac{r}{\sqrt{2}} \) back into the gravitational intensity formula: \[ G_P = \frac{Gm \left(\frac{r}{\sqrt{2}}\right)}{(r^2 + \left(\frac{r}{\sqrt{2}}\right)^2)^{3/2}} \] Calculating \( r^2 + \frac{r^2}{2} = \frac{3r^2}{2} \): \[ G_P = \frac{Gm \left(\frac{r}{\sqrt{2}}\right)}{\left(\frac{3r^2}{2}\right)^{3/2}} = \frac{Gm \left(\frac{r}{\sqrt{2}}\right)}{\left(\frac{3\sqrt{3}}{8} r^3\right)} = \frac{8Gm}{3\sqrt{3}r^2} \] ### Final Result Thus, the maximum gravitational intensity on the axis of the ring is: \[ G_P = \frac{2Gm}{3\sqrt{3}r^2} \]
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