Playing around with the calculator on the previous page (and at the bottom of this page) should
have convinced yourself of the following:
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In fact, let's denote this limiting matrix by L% (which
is supposed to look like L to the power infinity, because that's what it actually is).
Since
infinity + 1 = infinity (bear with me here; if you can handle the idea of infinity being a number, then this is simpler than the more rigorous mathematical treatment), we expect L% = LL% = L%L. And in fact, multiplying L% from the left or right by L yields L% back again. Continuing on in this vein, recall that n(t) = Lt n(0), where n(t) is the column matrix of 3 populations nx(t). Therefore, let n(%) = L% n(0), which is the column of populations after an infinite number of generations (which won't happen until the year 2089). |
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Performing the matrix multiplication we get n1(%) = 2n2(%) = 2n3(%) = (n1(0)/2 + 2n2(0)/3 + n3(0)/3). (So n1(%) + 2n2(%) + n3(%) = (n1(0) + 4n2(0)/3 + 2n3(0)/3).) This explains what we should have observed playing with the calculator re the ratios of the 1, 2 and 3 year old populations for large t. Note that L n(%) = LL% n(0) = L%+1 n(0) = L% n(0) = n(%),.................(eigenvector equation), and that explains why if n1(t) = 2n2(t) = 2n3(t), then n(t+1) = L n(t) = n(t).
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The general form of a matrix eigenvalue equation is A v = µ v where A is an nxn matrix, v an nx1 matrix (vector), and µ a number. v is called the eigenvector, and µ its eigenvalue. Note that if v is an eigenvector of some matrix A, then so is cv for any constant c; so eigenvectors determine eigen-"directions". In the L-eigenvector equation written above, n(%) is the eigenvector, and µ = 1 is the corresponding eigenvalue. (There are two other eigenvalues for L, but they are complex numbers with nonzero imaginary components, and they won't be of interest to us.) |
The eigenvalue
µ = 1 is quite special, and it is repsonsible for the fact that the nine components of
L% are finite real numbers, and for the fact that whatever populations nx(0)
we may start with, after a large number of generations we will settle near the stable values of
nx(%), which are finite. On the next page we'll construct a new set of fx (but leave the Px the same), resulting in an eigenvalue bigger than 1, and consequently exponential growth. |
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