- #36
lxman
- 77
- 0
Alright, here is what I have got (I know, I'm rocketing along like a herd of turtles):
The slope of the hypotenuse of the triangle is:
[tex]y=\sqrt{3}x-\frac{2h}{3}[/tex]
h of course is the length of the side along the y axis
Solving for x I get:
[tex]x=\frac{y+\frac{2h}{3}}{\sqrt{3}}[/tex]
Now, you state that
[tex]2\int_{-\frac{2h}{3}}^{\frac{h}{3}}y^{2}x(y)\,\mathmr{d}y[/tex]
So, what we are doing here is taking smaller and smaller sections of the triangle parallel to the x axis. Based on the principle that a force applied at a distance from a fulcrum varies as to its effect according to the square of the distance, that explains the y^2 term. Then the x(y) term gives us the area of our infinitesimally small interval. The product is the second moment of area of each tiny subdivision. Integrating this with h=[tex]\sqrt{3}[/tex], I arrive at the following result:
[tex]\frac{1}{2\sqrt{3}}[/tex]
I am using a CAS from this point, so I would have a difficult time writing out the full equation. Then, I evaluate my equation at [tex]\sqrt{3}-\frac{3}{4}[/tex] and I get:
A big old nasty fraction which my latex skills can't handle - but a numerical approximation is [tex]\approx[/tex] .03
So, subtracting one from the other, I come up with a result of [tex]\approx[/tex] .259
I certainly hope that I have gotten it right this time.
Once I receive confirmation that I have in fact followed the process correctly, I will be back with a few more questions. If I am wrong, however, I will continue to try.
Once again, thank you all for your wonderful support.
The slope of the hypotenuse of the triangle is:
[tex]y=\sqrt{3}x-\frac{2h}{3}[/tex]
h of course is the length of the side along the y axis
Solving for x I get:
[tex]x=\frac{y+\frac{2h}{3}}{\sqrt{3}}[/tex]
Now, you state that
[tex]2\int_{-\frac{2h}{3}}^{\frac{h}{3}}y^{2}x(y)\,\mathmr{d}y[/tex]
So, what we are doing here is taking smaller and smaller sections of the triangle parallel to the x axis. Based on the principle that a force applied at a distance from a fulcrum varies as to its effect according to the square of the distance, that explains the y^2 term. Then the x(y) term gives us the area of our infinitesimally small interval. The product is the second moment of area of each tiny subdivision. Integrating this with h=[tex]\sqrt{3}[/tex], I arrive at the following result:
[tex]\frac{1}{2\sqrt{3}}[/tex]
I am using a CAS from this point, so I would have a difficult time writing out the full equation. Then, I evaluate my equation at [tex]\sqrt{3}-\frac{3}{4}[/tex] and I get:
A big old nasty fraction which my latex skills can't handle - but a numerical approximation is [tex]\approx[/tex] .03
So, subtracting one from the other, I come up with a result of [tex]\approx[/tex] .259
I certainly hope that I have gotten it right this time.
Once I receive confirmation that I have in fact followed the process correctly, I will be back with a few more questions. If I am wrong, however, I will continue to try.
Once again, thank you all for your wonderful support.