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If the unit of length be doubled then th...

If the unit of length be doubled then the numerical value of the universal gravitation constant G will become (with respect to present value)

A

Double

B

Half

C

`8` times

D

`1//8` times

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The correct Answer is:
To solve the problem, we need to analyze how the universal gravitational constant \( G \) changes when the unit of length is doubled. ### Step-by-Step Solution: 1. **Understand the formula for \( G \)**: The universal gravitational constant \( G \) has the dimensional formula: \[ G = \frac{F \cdot r^2}{m_1 \cdot m_2} \] where \( F \) is the gravitational force, \( r \) is the distance between the masses \( m_1 \) and \( m_2 \). 2. **Identify the dimensions of \( G \)**: The dimensional formula for \( G \) is: \[ [G] = M^{-1} L^3 T^{-2} \] where \( M \) is mass, \( L \) is length, and \( T \) is time. 3. **Change in units**: If the unit of length is doubled, we denote the new unit of length as \( L_2 = 2L_1 \). 4. **Substituting the new length into the formula**: The new value of \( G \) can be expressed as: \[ G_2 = \frac{F \cdot (L_2)^2}{m_1 \cdot m_2} \] Since \( L_2 = 2L_1 \), we have: \[ G_2 = \frac{F \cdot (2L_1)^2}{m_1 \cdot m_2} = \frac{F \cdot 4L_1^2}{m_1 \cdot m_2} \] 5. **Relate the new \( G \) to the old \( G \)**: Since the force \( F \) remains the same, we can express \( G_2 \) in terms of \( G_1 \): \[ G_2 = 4 \cdot \frac{F \cdot L_1^2}{m_1 \cdot m_2} = 4G_1 \] 6. **Final expression**: Therefore, when the unit of length is doubled, the new value of \( G \) becomes: \[ G_2 = \frac{G_1}{4} \] ### Conclusion: The numerical value of the universal gravitational constant \( G \) will become \( \frac{1}{4} \) of its present value when the unit of length is doubled.

To solve the problem, we need to analyze how the universal gravitational constant \( G \) changes when the unit of length is doubled. ### Step-by-Step Solution: 1. **Understand the formula for \( G \)**: The universal gravitational constant \( G \) has the dimensional formula: \[ G = \frac{F \cdot r^2}{m_1 \cdot m_2} ...
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