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The bodies of mass 100 kg and 8100 kg ar...

The bodies of mass 100 kg and 8100 kg are held at a distance of 1 m. The gravitational field at a point on the line joining them is zero. The gravitational potential at that point in J/kg is (G=`6.67xx10^(-11)Nm^2//kg^2`)

A

`-6.67xx10^(-7)`

B

`-6.67xx10^(-10)`

C

`-13.34xx10^(-7)`

D

`-6.67xx10^(-9)`

Text Solution

AI Generated Solution

The correct Answer is:
To solve the problem, we need to find the gravitational potential at a point on the line joining two masses (100 kg and 8100 kg) where the gravitational field is zero. ### Step-by-Step Solution: 1. **Identify the Masses and Distance**: - Let mass \( m_1 = 100 \, \text{kg} \) and mass \( m_2 = 8100 \, \text{kg} \). - The distance between the two masses is \( d = 1 \, \text{m} \). 2. **Determine the Point Where Gravitational Field is Zero**: - Let the distance from \( m_1 \) to the point be \( x \). - Therefore, the distance from \( m_2 \) to the point will be \( 1 - x \). 3. **Set Up the Equation for Gravitational Fields**: - The gravitational field \( E \) due to a mass \( m \) at a distance \( r \) is given by: \[ E = \frac{Gm}{r^2} \] - At the point where the gravitational field is zero, the gravitational fields due to both masses must be equal: \[ \frac{G \cdot 100}{x^2} = \frac{G \cdot 8100}{(1 - x)^2} \] - We can cancel \( G \) from both sides: \[ \frac{100}{x^2} = \frac{8100}{(1 - x)^2} \] 4. **Cross-Multiply to Solve for x**: - Cross-multiplying gives: \[ 100(1 - x)^2 = 8100x^2 \] - Expanding the left side: \[ 100(1 - 2x + x^2) = 8100x^2 \] \[ 100 - 200x + 100x^2 = 8100x^2 \] - Rearranging gives: \[ 100 - 200x - 8000x^2 = 0 \] - Dividing through by 100: \[ 1 - 2x - 80x^2 = 0 \] - Rearranging: \[ 80x^2 + 2x - 1 = 0 \] 5. **Use the Quadratic Formula**: - The quadratic formula is given by: \[ x = \frac{-b \pm \sqrt{b^2 - 4ac}}{2a} \] - Here, \( a = 80 \), \( b = 2 \), and \( c = -1 \): \[ x = \frac{-2 \pm \sqrt{2^2 - 4 \cdot 80 \cdot (-1)}}{2 \cdot 80} \] \[ x = \frac{-2 \pm \sqrt{4 + 320}}{160} \] \[ x = \frac{-2 \pm \sqrt{324}}{160} \] \[ x = \frac{-2 \pm 18}{160} \] - This gives two solutions: \[ x = \frac{16}{160} = 0.1 \, \text{m} \quad \text{(valid)} \] \[ x = \frac{-20}{160} \quad \text{(not valid)} \] 6. **Calculate the Gravitational Potential**: - The gravitational potential \( V \) at a distance \( r \) from a mass \( m \) is given by: \[ V = -\frac{Gm}{r} \] - The total gravitational potential at the point is the sum of the potentials due to both masses: \[ V = V_1 + V_2 = -\frac{G \cdot 100}{0.1} - \frac{G \cdot 8100}{0.9} \] - Substituting \( G = 6.67 \times 10^{-11} \): \[ V = -\frac{6.67 \times 10^{-11} \cdot 100}{0.1} - \frac{6.67 \times 10^{-11} \cdot 8100}{0.9} \] \[ = -6.67 \times 10^{-10} - 7.41 \times 10^{-10} \] \[ = -1.407 \times 10^{-9} \, \text{J/kg} \] 7. **Final Answer**: - The gravitational potential at that point is: \[ V = -6.67 \times 10^{-7} \, \text{J/kg} \]
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