Find a curve $\gamma$ satisfying $\int_\gamma y^3 \sin^2(x) \, dx - x^5 \cos^2(y) \, dy = 0$ Let a closed curve, $\gamma$, be parameterized by a function $f : [0, 1] → \mathbb{R}^2$ with a continuous derivative and f(0) = f(1). Suppose that
$$ \int_\gamma y^3 \sin^2(x) \, dx - x^5 \cos^2(y) \, dy = 0 $$
Show that there exists a pair $\{x, y\} \neq \{0, 1\}$ with $x \neq y$ and $f(x) = f(y)$. Give an example of a curve satisfying above requirement and the only pairs $\{x, y\}$ with $x \neq y$ and $f(x) = f(y)$ are subsets of $\{0, 1/2, 1\}$.
My attempts: I know how to prove that there are other pairs of $\{x,y\}$ such that $f(x) = f(y)$. But I have no idea how to construct such curve $\gamma$. I think that by using Green's Formula, I will have
$$\iint_D (5x^4 \cos^2 (y) + 3y^2 \sin^2(x))\, dx\, dy = 0. $$
What else information could I derive from above?
 A: Here I would like to answer my own question. Here I would like to thank @TedShifrin for helping me with this.
First, we show that there exists another pair of $\{x,y\} \neq \{0,1\}$ such that $f(x) = f(y)$. This indeed requires us to show that $\gamma$ is not simple, i.e., it is self-crossed. We could prove it by contradiction: suppose $\gamma$ is simple. Then by Green's Formula, we have that
$$\int\int_D \left(5x^4 \cos^2(y) + 3y^2 \sin^2(x) \right)dxdy = 0.$$
Define the integrand is $F(x,y) := 5x^4 \cos^2(y) + 3y^2 \sin^2(x).$ Note that $ F(x,y) \geq 0$ for all $(x,y) \in \mathbb{R}^2$, so $\int\int_D \left(5x^4 \cos^2(y) + 3y^2 \sin^2(x) \right)dxd y > 0$ for any region $D$ enclosed by simple closed curve $\gamma$. (We could argue this by considering a small neighborhood inside $D$ with $(x,y) \in D$ such that $F(x,y) > 0$, and using the continuity) This is a contradiction, and we proved that $\gamma$ is not simple.
To construct an example, notice that $F(x,y) = F(-x,-y)$. Therefore, we could let $\Gamma: [0, \frac{1}{2}] \to \mathbb{R}^2$ be a closed, simple curve with continuous derivatives such that $\Gamma(0) = \Gamma(\frac{1}{2})$. Define $f$, the parametrization of $\gamma$ as follows: $f(x) = \Gamma(x)$ for $x \in [0,\frac{1}{2}]$ and $f(x) = -\Gamma(1-x)$ for $x \in (\frac{1}{2},1]$. By using Chain Rule, we know that $f$ is continuously differentiable; $f([0,\frac{1}{2}])$ and $f([\frac{1}{2},1])$ are simple and closed. Thus,
$$\int\int_\gamma F  = \int\int_{f([0,\frac{1}{2}])} F + \int\int_{f([\frac{1}{2},1])} F = \int\int_{f([0,\frac{1}{2}])} F + \int\int_{-f([0,\frac{1}{2}])} F = 0.$$ 
For a concrete example, we could consider a unit circle centered at $(1,0)$: $\Gamma(t) = (\cos(4\pi t + \pi)+1, \sin(4\pi t + \pi))$, and extend it oddly.
