Test of Second Partials - Proof

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The discussion focuses on the Second Derivative Test for functions of two variables, specifically the conditions under which a critical point (a,b) is classified as a local maximum or minimum. It establishes that if D > 0 and fxx < 0, then f(a,b) is a local maximum; if D > 0 and fxx > 0, then f(a,b) is a local minimum. The determinant D is defined as D = fxx(a,b)fyy(a,b) - [fxy(a,b)]2. The proofs rely on the continuity of second partial derivatives and the behavior of the function near the critical point.

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  • Knowledge of Taylor series expansion for functions of two variables
  • Basic concepts of matrix representation of linear transformations
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Can anyone give me a proof or some kind of general explanation about why there is a local max at (a,b) if D>0 and fxx<0, a min if D>0 and fxx>0, etc. My textbook doesn't give any kind of explanation at all and I'm just a little curious as to why it works.
 
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Second Derivatives Test:
Suppose the second partial derivatives of f are continuous on a disk with center (a,b), and suppose that f_x(a,b)=0 and f_y(a,b)=0 [that is, (a,b) is a critical point of f]. Let

D=D(a,b)=f_{xx}(a,b)f_{yy}(a,b)-[f_{xy}(a,b)]^2

(a) If D>0 and f_{xx}(a,b)&gt;0, then f(a,b) is a local minimum.
(b) If D>0 and f_{xx}(a,b)&lt;0, then f(a,b) is a local maximum.
(c) If D<0 and f_{xx}(a,b)&gt;0, then f(a,b) is not a local maximum or minimum.

Proof of part (a):

We compute the second-order directional derivative of f in the direction of \vec u = \langle h, k \rangle. The first-order derivative is given by:
D_uf=f_xh+f_yk \quad \mbox{(from a different theorem)}
Applying this theorem a second time, we have:
<br /> \begin{eqnarray}<br /> D^2_uf &amp; = &amp; D_u(D_uf)=\frac{\partial}{\partial x}(D_uf)h+\frac{\partial}{\partial y}(D_uf)k \nonumber \\<br /> &amp; = &amp; (f_{xx}h+f_{yx}k)h+(f_{xy}h+f_{yy}k)k \nonumber\\<br /> &amp; = &amp; f_{xx}h^2+2f_{xy}hk+f_{yy}k^2 \mbox{(by Clairaut&#039;s theorem)}\nonumber<br /> \end{eqnarray}<br />

If we complete the square in this expression, we obtain:
D_u^2f=f_{xx}\left(h+\frac{f_{xy}}{f_{xx}}k\right)^2+\frac{k^2}{f_{xx}}(f_{xx}f_{yy}-f^2_{xy}) \quad \mbox(&lt;- Equation 1)
We are given that f_{xx}(a,b)&gt;0 and D(a,b)&gt;0. But f_{xx} and D=f_{xx}f_{yy}-f^2_{xy} are continuous functions, so there is a disk B with center (a,b) and radius \delta&gt;0 such that f_{xx}&gt;0 and D&gt;0 whenever (x,y) is in B. Therefore, by looking at Equation 1, we see that D_u^2f(x,y)&gt;0 whenever (x,y) is in B. This means that if C is the curve obtained by intersecting the graph of f with the vertical plane through P(a,b,f(a,b)) in the direction of \vec u, then C is concave upward on an interval of length 2\delta. This is true in the direction of every vector \vec u, so if we restrict (x,y) to lie in B, the graph lies above its horizontal tangent plane at P. Thus f(x,y)\geq f(a,b) whenever (x,y) is in B. This shows that f(a,b) is a local minimum.


Parts (b) and (c) have similar proofs.
 
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Notice that what Galileo is really doing is expanding f(x,y) in a Taylor's series with two variables. The derivatives at a critical point are 0 so there are no first power terms. For x, y very close to the critical point, we can ignore higher powers so we have only the constant term (the value of f AT the critical point) and the quadratic terms. We can always change the coordinate system to eliminate any "xy" term and have left ax2+ by2 (with a, b, positive, negative, or 0). If both a and b are positive, that's a minimum, if negative, maximum. If either is 0, we need to look at higher powers.

What's REALLY happening is that, with a real valued function of of R2 to R, the second derivative is a linear function from R2 to R2 which can be represented as a 2 by 2 matrix (the entries are: first row fxx, fxy, second row fyx, fyy).

Since that is a symmetric matrix we can always change the coordinate system to make that a diagonal matrix resulting in the "ax2+ b2" above (a, b are the diagonal elements). Of course the determinant of such a matrix is ab so everything depends upon whether that determinant is positive or negative. But the determinant is independent of changing the coordinate system so we can just look at the determinant of the original matrix: D= (fxxfyy-fxy2).
 
The second derivative test can seem rather tricky and abstract to begin with, but, as HallsofIvy said, what you really get out of it, is either:
1) Locally, your graph looks like a paraboloid expanding upwards (i.e, you've got positive curvatures and a minimum point)
2) Locally, your graph looks like a paraboloid expanding downwards (i.e, you've got negative curvatures and a maximum point)
3) Locally, your graph looks like a "saddle", neither maximum nor minimum.
4) Second derivatives test is insufficient in elucidating local behaviour (i.e, you must look on higher derivatives, (assuming those exist))
 
The book claims the answer is that all the magnitudes are the same because "the gravitational force on the penguin is the same". I'm having trouble understanding this. I thought the buoyant force was equal to the weight of the fluid displaced. Weight depends on mass which depends on density. Therefore, due to the differing densities the buoyant force will be different in each case? Is this incorrect?

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