align fix; theorem style; condition number
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@@ -302,20 +302,20 @@ We could also do the above problem symbolically with the aid of `SymPy`. Here ar
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```{julia}
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@syms 𝐰::real 𝐡::real
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@syms w₀::real h₀::real
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𝐀₀ = 𝐰 * 𝐡 + pi * (𝐰/2)^2 / 2
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𝐏erim = 2*𝐡 + 𝐰 + pi * 𝐰/2
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𝐡₀ = solve(𝐏erim - 20, 𝐡)[1]
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𝐀₁ = 𝐀₀(𝐡 => 𝐡₀)
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𝐰₀ = solve(diff(𝐀₁,𝐰), 𝐰)[1]
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A₀ = w₀ * h₀ + pi * (w₀/2)^2 / 2
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Perim = 2*h₀ + w₀ + pi * w₀/2
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h₁ = solve(Perim - 20, h₀)[1]
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A₁ = A₀(h₀ => h₁)
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w₁ = solve(diff(A₁,w₀), w₀)[1]
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```
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We know that `𝐰₀` is the maximum in this example from our previous work. We shall see soon, that just knowing that the second derivative is negative at `𝐰₀` would suffice to know this. Here we check that condition:
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We know that `w₀` is the maximum in this example from our previous work. We shall see soon, that just knowing that the second derivative is negative at `w₀` would suffice to know this. Here we check that condition:
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```{julia}
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diff(𝐀₁, 𝐰, 𝐰)(𝐰 => 𝐰₀)
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diff(A₁, w₀, w₀)(w₀ => w₁)
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```
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As an aside, compare the steps involved above for a symbolic solution to those of previous work for a numeric solution:
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@@ -614,7 +614,7 @@ We see two terms: one with $x=L$ and another quadratic. For the simple case $r_0
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```{julia}
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solve(q(r1=>r0), x)
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solve(q(r1=>r0) ~ 0, x)
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```
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Well, not so fast. We need to check the other endpoint, $x=0$:
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@@ -632,7 +632,7 @@ Now, if, say, travel above the line is half as slow as travel along, then $2r_0
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```{julia}
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out = solve(q(r1 => 2r0), x)
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out = solve(q(r1 => 2r0) ~ 0, x)
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```
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It is hard to tell which would minimize time without more work. To check a case ($a=1, L=2, r_0=1$) we might have
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@@ -1372,11 +1372,12 @@ solve(x/b ~ (x+a)/(b + b*p), x)
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With $x = a/p$ we get by Pythagorean's theorem that
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$$
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\begin{align*}
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c^2 &= (a + a/p)^2 + (b + bp)^2 \\
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&= a^2(1 + \frac{1}{p})^2 + b^2(1+p)^2.
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\end{align*}
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$$
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The ladder problem minimizes $c$ or equivalently $c^2$.
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