How Do You Calculate the Center of Mass for an Isosceles Triangle?

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SUMMARY

The center of mass for an isosceles triangle with two equal sides of length 'a' and a base of length 'b' can be calculated using geometric principles rather than complex calculus. The centroid, which represents the center of mass for uniform density, is located at the average of the vertices' coordinates. Specifically, if the triangle's vertices are positioned at (0, 0), (b, 0), and (a/2, y), where 'y' is determined to maintain the side lengths, the centroid coordinates are ((0 + b + a/2)/3, (0 + 0 + y)/3). This approach simplifies the problem significantly.

PREREQUISITES
  • Understanding of basic geometry, specifically properties of triangles.
  • Familiarity with the concept of centroids and their calculation.
  • Knowledge of coordinate systems and slope-intercept form.
  • Basic calculus for integration, though not strictly necessary for this problem.
NEXT STEPS
  • Study the properties of centroids in various geometric shapes.
  • Learn how to derive the centroid formula for different types of triangles.
  • Explore the application of integration in calculating areas and centroids.
  • Investigate the use of polar coordinates in geometric problems.
USEFUL FOR

Students in physics or mathematics, educators teaching geometry, and anyone interested in understanding the principles of calculating centroids in geometric figures.

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Homework Statement


Find the center of mass of a triangle with two equal sides of length a. The triangle's third side is length b and it has a uniform mass of M.


Homework Equations


R = \frac{1}{M} \int dm \vec{r}
dm = \frac{M}{A}
A = \frac{1}{2}base*height


The Attempt at a Solution


Right now I have my triangle set up with one of the "a" length sides on the x-axis. I'm having trouble defining the y limit in the integral:
X = \frac{1}{M} \rho \int_{0}^{a} x dx \int dy​
I know that it has to have length "b" for the triangle I have drawn. I also found that it was equal to tan\theta_{1}, but I need it in terms of x to complete the integral. It's that or change variables. I've also been throwing around the idea of doing this in polar coordinates.
 
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I don't see why you are going through all this trouble when you can transform this into a one-dimensional problem.

The triangle's center of mass is obviously down the perpendicular bisector of side b. Therefore, you can just calculate the problem as though all the mass is concentrated on that bisector.

To do that, put the triangle such that b is on the y-axis and its perpendicular bisector is on the x axis. You'll end up with two lines beginning at y=b/2 and converging at x=a. These lines can be found in slope-intercept form as y=∓b/(2a)x±b/2. Considering that this simplification requires dictates that the mass is completely concentrated along the x axis, you can just do a single integral in which y=-(b/a)x+b from x=0 to a. (This gives you the mass, if you really wanted to do it by calculus.)

Go back and find the point x=c at which x ∫0c y dx = ∫ca y dx = 1/2 ∫0a y dx.
 
Frankly, this isn't a "physics" problem at all! The "center of mass" of an object with uniform density is really a geometric object, the "centroid". And it is not too difficult to show that the centroid of a triangle is the point whose coordinates are the average of the coordinates of the three vertices:
If a triangle has vertices at (a, b, c), (d, e, f), and (g, h, i) then its centroid is at ((a+ d+ g)/3, (b+ e+ h)/3, (c+ f+ i)/3).

I would set up a coordinate system so that one end of the "dd side", of length b, is at the origin, and the other end at (b, 0). The third vertex will be at (a/2, y) where y is chosen so that the two sides have length a.
 

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