Mathematical Food for Thought

 
 
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    Serves a Daily Special and an All-You-Can-Eat Course in Problem Solving. Courtesy of me, Jeffrey Wang.
 
Symmetry For The Win. Topic: Calculus. October 30th, 2006

Problem: Evaluate the improper integral  I = \displaystyle \int_0^{\pi} \ln{(\sin{x})} dx .

Solution: As the topic suggests, we will look for a symmetry to simplify the problem. Notice the identity  \displaystyle \int_0^a f(x) dx = \int_0^a f(a-x) dx (since we’re just integrating across the interval from different “directions.” Using this, we have

 \displaystyle I = \int_{0}^{\frac{\pi}{2}}\ln{(\sin{x})}dx = \int_{0}^{\frac{\pi}{2}}\ln{\left(\sin{\left(\frac{\pi}{2}-x\right)}\right)}dx = \int_{0}^{\frac{\pi}{2}}\ln{(\cos{x})}dx .

Adding the old integral to the new one, we have

 \displaystyle 2I = \int_{0}^{\frac{\pi}{2}}\ln{(\sin{x})}dx+\int_{0}^{\frac{\pi}{2}}\ln{(\cos{x})}dx = \int_{0}^{\frac{\pi}{2}}\ln{\left(\frac{1}{2}\sin{2x}\right)}dx

from the property of logs and the double-angle identity (here it is again!). But in fact this expression is simply

 \displaystyle 2I =-\frac{\pi}{2}\ln{2}+\frac{1}{2}\int_{0}^{\pi}\ln{(\sin{u})}du (*)

by the substitution  u = 2x . Taking into the account of the symmetry of  \sin{x} from  0 to  \pi , we get  \sin{x} = \sin{(\pi-x)} so

 \displaystyle \frac{1}{2}\int_{0}^{\pi}\ln{(\sin{u})}du = \int_{0}^{\frac{\pi}{2}}\ln{(\sin{u})}du = I .

Plugging back into (*) we obtain  \displaystyle 2I =-\frac{\pi}{2}\ln{2}+I so we get  I = -\frac{\pi}{2}\ln{2} . QED.

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Comment: The function is not nice to actually integrate; it involves the polylogarithm function if you try here. This is an important example of how symmetry can help a ton in integration because there are so many functions that cannot be integrated with elementary functions but can be evaluated over an interval through different techniques.

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Practice Problem: Evaluate  \displaystyle \int_0^{\frac{\pi}{2}} \sin^4{x} dx without actually finding the antiderivative.

Out Of Place Trig. Topic: Geometry/Trigonometry. Level: AMC/AIME. October 29th, 2006

Problem: (2006-2007 Warm-Up 4) Two sides of a triangle are  4 and  |\cos{\theta}| and the angle between them is  \theta . If  0 < \theta < \pi , what is the maximum area of the triangle?

Solution: Well, given two sides and the angle between them, there is only one formula for the area of a triangle that comes to mind.  [ABC] = \frac{1}{2}ab \sin{(\angle C)} . So plugging this in, we get the area to be

 \frac{1}{2} (4) |\cos{\theta}| \sin{\theta} = 2 \sin{\theta} |\cos{\theta}| .

By the double-angle identity, this is equal to

 |\sin{(2\theta)}|

for  0 < \theta < \pi . But the maximum of this is clearly  1 and it is obtained when  \theta = \frac{\pi}{4}, \frac{3 \pi}{4} . QED.

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Comment: This problem shouldn’t have been too hard; finding that specific formula for the area of the triangle could have been derived by drawing an altitude. And the double-angle identity should always be known. Lastly, maximizing the sine function is a given.

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Practice Problem: (2006 Skyview) If  \sin{x} = \frac{3}{5} and  \cos{x} = \frac{4}{5} , what is  \sin{(3x)} ?

Bellevue Wins First At Skyview! October 28th, 2006
Square Sum Stuff. Topic: Polynomials/S&S. Level: AMC/AIME. October 27th, 2006

Problem: Evaluate the summation

 \displaystyle \sum_{k=1}^{\infty} \frac{k^2}{2^k} = \frac{1^2}{2^1}+\frac{2^2}{2^2}+\frac{3^2}{2^3}+\frac{4^2}{2^4}+\cdots .

Solution: Here’s a technique that will help you evaluate infinite series that are of the form polynomial over exponential. It’s based on the idea of finite differences:

If  P is a polynomial with integer coefficients of degree  n then

 P(x+1)-P(x)

is a polynomial of degree  n-1 (not hard to show; just think about it).

So let

 S = \frac{1^2}{2^1}+\frac{2^2}{2^2}+\frac{3^2}{2^3}+\frac{4^2}{2^4}+\cdots .

Then consider  2S by simply multiplying each term by  2 :

 2S = 1^2+\frac{2^2}{2^1}+\frac{3^2}{2^2}+\frac{4^2}{2^3}+\cdots .

And now find the difference  2S-S = S by subtracting the terms with equal denominators. We get

 S = 2S-S = 1+\frac{2^2-1^2}{2^1}+\frac{3^2-2^2}{2^2}+\frac{4^2-3^2}{2^3}+\cdots

 S = 1+\frac{3}{2^1}+\frac{5}{2^2}+\frac{7}{2^3}+\cdots .

Notice that the numerator is now a polynomial of degree  1 instead of  2 . Repeating this, we have

 2S = 2+3+\frac{5}{2^1}+\frac{7}{2^2}+\cdots

and

 S = 2S-S = 2 + 2 + \frac{5-3}{2^1}+\frac{7-5}{2^2}+\cdots

 S = 2 + (2 + 1+\frac{1}{2}+\cdots) .

Notice that the latter part is just a geometric series which sums to

 2 + 1 + \frac{1}{2} + \cdots = 4

so  S = 2+4 = 6 . QED.

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Comment: The method of finite differences is extremely useful and is basically a simplified version of calculus –  P(x+1)-P(x) \approx P^{\prime}(x) in a very approximating sense. It’s a good thing to know, though, because then you have a better understanding of how polynomials work.

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Practice Problem: Let  P be a polynomial with integer coefficients. Using the method of finite differences, predict the degree of  P .

 P(1) = 1 \mbox{  } P(2) = 9 \mbox{  } P(3) = 20 \mbox{  } P(4) = 36 \mbox{  } P(5) = 59 \mbox{  } P(6) = 91 .

Serious Substitution. Topic: Calculus. October 25th, 2006

Problem: Use the substitution  z = \sqrt{x} to solve the differential equation  4x \frac{d^2y}{dx^2}+2 \frac{dy}{dx}+y = 0 .

Solution: Well, let’s do what it says. From the chain rule, we have

 \displaystyle \frac{dy}{dz} = \frac{dy}{dx} \cdot \frac{dx}{dz} = 2z \frac{dy}{dx} .

Then we also have by the product rule and chain rule again

 \displaystyle \frac{d^2y}{dz^2} = 2 \frac{dy}{dx}+2z \frac{d^2y}{dx^2} \cdot \frac{dx}{dz} = \frac{1}{z} \cdot \frac{dy}{dz}+4z^2 \frac{d^2y}{dx^2} .

So we can make the substitutions

 \displaystyle 4x \frac{d^2y}{dx^2} = 4z^2 \frac{d^2y}{dx^2} = \frac{d^2y}{dz^2}-\frac{1}{z} \cdot \frac{dy}{dz}

and

 \displaystyle \frac{dy}{dx} = \frac{1}{2z} \cdot \frac{dy}{dz}

to obtain the differential equation

 \frac{d^2y}{dz^2}-\frac{1}{z} \cdot \frac{dy}{dz} + 2 \cdot \frac{1}{2z} \cdot \frac{dy}{dz}+y = \frac{d^2y}{dz^2}+y = 0 .

But we know the solution to this is  y = C_1 \cos{z}+C_2 \sin{z} so our final solution is

 y = C_1 \cos{\sqrt{x}}+C_2 \sin{\sqrt{x}} .

QED.

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Comment: This substitution is, of course, not really natural but was actually found after solving the ODE in another way. Fortunately, it simplifies the problem rather greatly and seems to be a useful technique to look out for.

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Practice Problem: Find another way to solve the differential equation.

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