I am trying to intuitively understand why the polar equation $r=(\cos(\theta))^{0.1}$ has the following shape compared to the circular $r=\cos(\theta)$. I see that the figure should have a greater area, as the values of $\cos$ between $1$ and $0$ will be increased when being raised to powers less than one. However, as to why the graph possesses the following curvature, I am at a loss to understand from the perspective of the qualities of a root function. I have tried so far thinking of the rate at which $x^{0.1}$ increases. I would appreciate an explanation as to why the shape is like this.
Thanks


I think that we can perceive what is going on considering the more general case of $$f_n(x)=\sqrt[n]{\cos (x)} \qquad \text{for}\qquad -\frac \pi 2 \leq x \leq \frac \pi 2$$
Built around $x=0$, its series expansion is $$f_n(x)=1-\frac{1}{2 n}x^2+\frac{3-2 n }{24 n^2}x^4-\frac{16 n^2-30 n+15 }{720n^3 }x^6-$$ $$\frac{272 n^3-588 n^2+420 n-105 }{40320 n^4 }x^8+O(x^{10})$$ which reproduces quite well the function except around the bounds.
The second derivative being $\frac {-1}n$ at $x=0$ explains the tightening of the curve.
Similarly $$A_n=\int_{-\frac \pi 2}^{\frac \pi 2} \sqrt[n]{\cos (x)}\, dx=\sqrt{\pi } \,\frac{\Gamma \left(\frac{n+1}{2 n}\right)}{\Gamma \left(\frac{2 n+1}{2 n}\right)}$$ increases from $2$ (for $n=1$) up to $\pi^-$ if $n\to \infty$ (is the circle coming ?).
Asymptotically $$A_n=\pi \left(1-\frac{\log (2)}{n}+\frac{\pi ^2+3 \log ^2(4)}{24 n^2}+O\left(\frac{1}{n^3}\right)\right)$$