Christmas Math Problem Set 2017 - Turtle-dove Curves

Calculus Level 4

An elf in Santa's workshop is making Christmas decorations, with a mathematical twist! He is making paper cut-outs by graphing functions to look like Christmas-themed things. Right now, he is trying to create a graph that looks like a turtle-dove and is in the process of graphing its body. He is using the equation y = x 3 1 x , y=x^3\sqrt{1 \ - \ x}, which looks like the black curve in the graph below:

The elf likes the shape of the body but doesn't think the wing placed on it looks right (the red curve). In order to draw the optimal wing, he needs to find the area of the body lying in the first quadrant. Help the elf find the area of the body. If the area can be expressed as A B \frac{A}{B} , where A A and B B are coprime integers, enter your answer as A + B A + B .


This problem is part of Christmas Math Problem Set 2017 .


The answer is 347.

This section requires Javascript.
You are seeing this because something didn't load right. We suggest you, (a) try refreshing the page, (b) enabling javascript if it is disabled on your browser and, finally, (c) loading the non-javascript version of this page . We're sorry about the hassle.

2 solutions

Jack Ceroni
Dec 9, 2017

We can start by solving the equation x 3 1 x = 0 x^3 \ \sqrt{1 \ - \ x} \ = \ 0 , and see that the graph of the turtle-dove's body is positive in the interval [ 0 , 1 ] [0, \ 1] , since these are the solutions to this equation, and therefore are the roots. We can then realize that this is a textbook example of the beta function. We know that:

\text{B}(y, \ z) \ = \ \displaystyle\int_{0}^{1} \ x^{y \ - \ 1} \ (1 \ - \ x)^{z \ - \ 1} \ \text{dx} \tag*{}

To find the area of this section of the graph, we can simply evaluate the integral. Using the relationship:

\text{B}(y, \ z) \ = \ \dfrac{\Gamma (y) \ \Gamma (z)}{\Gamma (y \ + \ z)} \tag*{}

We can solve this integral. We can say that for the integral:

\displaystyle\int_{0}^{1} \ x^3 \ \sqrt{1 \ - \ x} \ \text{dx} \ \Rightarrow \ y \ = \ 4, \ z \ = \ \frac{3}{2} \tag*{}

Then this can be written as B ( 4 , 3 2 ) \text{B}(4, \ \frac{3}{2}) . This means that:

\text{B}(4, \ \frac{3}{2}) \ = \ \dfrac{\Gamma (4) \ \Gamma (\frac{3}{2})}{\Gamma (\frac{11}{2})} \tag*{}

We know that Γ ( x ) = ( x 1 ) ! \Gamma (x) \ = \ (x \ - \ 1)! and Γ ( x + 1 ) = x Γ ( x ) \Gamma (x \ + \ 1) \ = \ x \Gamma (x) . This means that we can start to simplify this expression. First of all, Γ ( 4 ) = ( 4 1 ) ! = 6 \Gamma (4) \ = \ (4 \ - \ 1)! \ = \ 6 . We can now use the reflection formula to find Γ ( 3 2 ) \Gamma (\frac{3}{2}) . The reflection formula is defined as:

\Gamma (x) \ \Gamma (1 \ - \ x) \ = \ \dfrac{\pi}{\sin (\pi x)} \tag*{}

We can begin to simplify Γ ( 3 2 \Gamma (\frac{3}{2} by seeing that it is equal to 1 2 Γ ( 1 2 ) \frac{1}{2} \ \Gamma (\frac{1}{2}) . We can then see that through the reflection formula:

\Gamma (\frac{1}{2}) \ \Gamma (\frac{1}{2}) \ = \ (\Gamma (\frac{1}{2}))^2 \ = \ \dfrac{\pi}{\sin (\frac{\pi}{2})} \ = \ \pi \tag*{}

This means that Γ ( 1 2 ) = π \Gamma (\frac{1}{2}) \ = \ \sqrt{\pi} . Finally, we can use the formula, Γ ( x + 1 ) = x Γ ( x ) \Gamma (x \ + \ 1) \ = \ x \Gamma (x) , to find the value of the denominator. We can continue to iterate using this formula to get: Γ ( 11 2 ) = 9 2 9 2 9 2 9 2 9 2 Γ ( 1 2 ) \Gamma (\frac{11}{2}) \ = \ \frac{9}{2} \ \cdot \ \frac{9}{2} \ \cdot \ \frac{9}{2} \ \cdot \ \frac{9}{2} \ \cdot \ \frac{9}{2} \ \Gamma (\frac{1}{2}) . We know that Γ ( 1 2 ) = π \Gamma (\frac{1}{2}) \ = \ \sqrt{\pi} . We can evalute the product of all of these terms to obtain 945 π 32 \frac{945 \sqrt{\pi}}{32} . We can plug this back into the original fraction to get 96 945 \frac{96}{945} . Simplifying this, we get 32 315 \frac{32}{315} . Adding the numerator and the denominator, we get 347 347 .

The problem asks for A = 0 1 x 3 1 x d x . A = \int_0^1 x^3\sqrt{1-x}\:dx. To simplify the integral, we try the substitution u = 1 x u = \sqrt{1 - x} . This gives d u = d x / 2 1 x du = -dx/2\sqrt{1-x} so that d x = 2 u d u dx = -2u\:du , and the limits of integration are flipped: A = 2 0 1 ( 1 u 2 ) 3 u 2 d u . A = 2 \int_0^1 (1-u^2)^3 u^2 \:du. Expand this: A = 2 0 1 ( u 2 3 u 4 + 3 u 6 u 8 ) d u = 2 [ 1 3 u 3 3 5 u 5 + 3 7 u 7 1 9 u 9 ] 0 1 = 2 ( 1 3 3 5 + 3 7 1 9 ) = 2 × 105 189 + 135 35 315 = 32 315 . A = 2\int_0^1 (u^2 - 3u^4 + 3u^6 - u^8)\:du = 2\left[\frac13u^3 - \frac 35 u^5 + \frac 37 u^7 - \frac 19 u^9\right]_0^1 \\ = 2\left(\frac 13 - \frac 35 + \frac 37 - \frac 19\right) = 2\times\frac{105 - 189 + 135 - 35}{315} = \frac{32}{315}. We therefore post our answer as 32 + 315 = 347 32 + 315 = \boxed{347} .

0 pending reports

×

Problem Loading...

Note Loading...

Set Loading...