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where A and B are the position vectors for the mass locations A and B
respectively, and P is the position vector for the centroid P .
If we extend the number of masses to three: m A ,m B and m C , which are
organized as a triangle, then we can write
m A
m A + m B + m C A +
m B
m A + m B + m C B +
m C
m A + m B + m C C
P =
(11.8)
The three multipliers of A , B and C are the barycentric coordinates of P
relative to the points A , B and C . Note that the number of coordinates is not
associated with the number of spatial dimensions, but the number of reference
points.
Now consider the scenario shown in Figure 11.5. If m A = m B = m C then
we can determine the location of A ,B and C as follows:
1. We begin by placing a fulcrum under A and mid-way along BC as shown
in Figure 11.6.
The triangle will balance because m B = m C and A is
1
2 a from C and
1
2 a
from B .
2. Now we place the fulcrum under B and mid-way along CA as shown in
Figure 11.7.
C
m C
b
B
a
A
P
C
m A
m B
A
B
c
Fig. 11.5. Three masses organized as a triangle.
m A
A
c
b
A
B
m B
m C
C
1
2 a
1
2 a
Fig. 11.6. Balancing the triangle along AA .
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