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THREE IDENTICAL MASS m ARE PLACED AT THE CORNER OF EQUILATERAL TRIANGLE OF SIDE a . THE GRAVITATIONAL POTENTIAL AT THE CENTROID OF THE TRIANGLE WILL BE WHAT ?

RAGINI SEIWAL , 7 Years ago
Grade 12
anser 1 Answers
Eshan

Last Activity: 7 Years ago

To find the gravitational potential at the centroid of an equilateral triangle formed by placing three identical masses (m) at its corners, we first need to understand a few key concepts related to gravitational potential and how it behaves in a system of point masses.

Gravitational Potential Defined

The gravitational potential (V) at a point in space due to a mass is given by the formula:

V = -G * M / r

where:

  • G = gravitational constant (approximately 6.674 × 10-11 N m2/kg2)
  • M = mass creating the gravitational field
  • r = distance from the mass to the point where the potential is being calculated

Geometry of the Problem

In our case, we have three identical masses located at the corners of an equilateral triangle with side length a. The centroid of this triangle is the point where all three medians intersect, and it is located at a distance of:

r = (a √3) / 3 from each vertex.

Calculating Gravitational Potential at the Centroid

The total gravitational potential at the centroid due to all three masses can be calculated by summing the potentials from each mass:

Total Gravitational Potential, Vtotal = V1 + V2 + V3

Since all three masses are identical and located at the same distance from the centroid, we can express this as:

Vtotal = 3 * V

Substituting the potential due to one mass:

V = -G * m / r

we get:

Vtotal = 3 * (-G * m / r)

Replacing r with (a √3) / 3, we have:

Vtotal = 3 * (-G * m / ((a √3) / 3))

Which simplifies to:

Vtotal = -9Gm / (a √3)

Final Result

Thus, the gravitational potential at the centroid of the triangle formed by three identical masses at its corners is:

Vcentroid = -9Gm / (a √3)

This negative value indicates that the gravitational potential is lower at the centroid due to the attractive nature of gravity, which draws the masses toward one another. This result not only reflects the influence of each mass but also illustrates the symmetry inherent in the system.

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