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Masses 1kg and 4kg are 6cm apart. The Po...

Masses 1kg and 4kg are 6cm apart. The Point along the line joining the masses where the gravitational field due to them is zero is

A

2cm from 1 kg mass

B

2cm from 4kg mass

C

4cm from 1kg mass

D

3cm from each mass

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To find the point along the line joining the masses where the gravitational field due to them is zero, we can follow these steps: ### Step 1: Understand the Setup We have two masses: - \( m_1 = 1 \, \text{kg} \) - \( m_2 = 4 \, \text{kg} \) They are separated by a distance of \( d = 6 \, \text{cm} \). ### Step 2: Define the Point of Interest Let \( P \) be the point where the gravitational field is zero. Let \( x \) be the distance from the 1 kg mass to point \( P \). Therefore, the distance from the 4 kg mass to point \( P \) will be \( (6 - x) \, \text{cm} \). ### Step 3: Set Up the Gravitational Field Equations The gravitational field \( E \) due to a mass \( m \) at a distance \( r \) is given by: \[ E = \frac{Gm}{r^2} \] Where \( G \) is the gravitational constant. At point \( P \), the gravitational fields due to both masses must be equal in magnitude but opposite in direction: \[ E_1 = E_2 \] Thus, \[ \frac{G m_1}{(6 - x)^2} = \frac{G m_2}{x^2} \] Since \( G \) appears on both sides, we can cancel it out: \[ \frac{m_1}{(6 - x)^2} = \frac{m_2}{x^2} \] ### Step 4: Substitute the Masses Substituting \( m_1 = 1 \, \text{kg} \) and \( m_2 = 4 \, \text{kg} \): \[ \frac{1}{(6 - x)^2} = \frac{4}{x^2} \] ### Step 5: Cross-Multiply Cross-multiplying gives: \[ 1 \cdot x^2 = 4 \cdot (6 - x)^2 \] Expanding the right side: \[ x^2 = 4(36 - 12x + x^2) \] \[ x^2 = 144 - 48x + 4x^2 \] ### Step 6: Rearrange the Equation Rearranging gives: \[ 0 = 4x^2 - x^2 - 48x + 144 \] \[ 0 = 3x^2 - 48x + 144 \] ### Step 7: Simplify the Quadratic Equation Dividing the entire equation by 3: \[ 0 = x^2 - 16x + 48 \] ### Step 8: Solve the Quadratic Equation Using the quadratic formula \( x = \frac{-b \pm \sqrt{b^2 - 4ac}}{2a} \): Here, \( a = 1, b = -16, c = 48 \): \[ x = \frac{16 \pm \sqrt{(-16)^2 - 4 \cdot 1 \cdot 48}}{2 \cdot 1} \] \[ x = \frac{16 \pm \sqrt{256 - 192}}{2} \] \[ x = \frac{16 \pm \sqrt{64}}{2} \] \[ x = \frac{16 \pm 8}{2} \] Calculating the two possible values: 1. \( x = \frac{24}{2} = 12 \, \text{cm} \) 2. \( x = \frac{8}{2} = 4 \, \text{cm} \) ### Step 9: Determine the Valid Solution Since \( x = 12 \, \text{cm} \) is outside the distance between the two masses, we discard it. Thus, the valid solution is: \[ x = 4 \, \text{cm} \] ### Conclusion The point along the line joining the masses where the gravitational field due to them is zero is at a distance of \( 4 \, \text{cm} \) from the \( 1 \, \text{kg} \) mass. ---
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