00:02
M1 is equal to m2 is equal to m3, and they're all equal to m and l1, l2, l3, and l4 are all equal to each other, and they all equal l over 4.
00:11
So we can model as a three degree of freedom system at the mass locations, y1, y2, y3 transpose.
00:22
Using flexibility, y is equal to a times f, or f is omega squared times m y, and m is equal to m times i.
00:32
So i minus omega squared a m times y is equal to zero, so omega squared is one over mu, where mu are eigenvalues of a .m.
00:46
For a fixed, fixed oil of renewing beam, the flexibility matrix had x equals l over 4, l over 2, and 3l over 4 would be l cubed over ei times the 3 by 3 matrix, 9 over 4.
01:02
4 ,096, 1 over 384, 13 over 12 ,288, 1 over 384, 1 over 192, 1 over 384, in row 313 over 1228, 1 over 384, and 9 over 4096.
01:28
And that gives omega sub i squared equals e, i over m l cubed times c sub i with our constants of about 124 .38877 .1413 and 2371 .6512.
01:57
That's ordered low to high frequency...