This appears to need a combination of exploration and confirmation.
To explore, graph the data. Polar plots work well. This one includes a smoothed version of the data (red line), which were obtained at 49 randomly selected angles:
There is just the slightest hint that the radii may have the alternative pattern: the smooth is just a bit greater than 1 for angles near 0 and just a bit less than 1 for angles near $\pi$. However, the scatter around the smooth is much greater than that, suggesting that this result may be due to chance.
A more powerful method of plotting these data to test this particular alternative is to match data obtained at angles $\theta$ with those obtained near angles $\theta+\pi$. (Although this halves the amount of data available for comparison, its amplification of the expected response more than makes up for that.) According to $H_0$, differences in radii will be scattered around $0$, whereas according to $H_1$, the differences will tend to be negative for small angles, pass through $0$ near $\pi/2$, and become positive. The next figure plots these differences. Specifically, it sorts the 49 observed values of $(\theta,r)$ and plots the 24 pairs $((\theta_{i} + \theta_{i+24} - \pi)/2, (r_{i} - r_{i+24}))$ for $i=1,2,\ldots,24$:
This approach opens the analysis to standard methods (exploratory and confirmatory) to check trends. For instance, we could perform a naive least-squares fit (of a linear trend). The result for these data, $p = 0.038$, might be considered significant evidence in favor of the alternative.
More sophisticated methods worth considering include:
- For exploration or confirmation, divide data into three groups for angles near $0$, $\pi/2$, and $\pi$. Compare the medians (or means) of differences of $r$ within each group. In this instance, ANOVA (as well as visual examination) indicates there are differences:
For confirmation, perform a multivariate least squares fit of the data to a few cosines (of periods $2\pi$ and $\pi$ to start). $H_0$ says that at most the constant term is significant; $H_1$ would be demonstrated by significance of any one of the odd-frequency terms.
For exploration or confirmation, fit periodic splines to the data.
Incidentally, these data were generated by the relation $r = 1 + \cos[\theta]^3/10$ with iid Normal error of standard deviation $1/10$ added. The figure shows this curve along with the null hypothesis (a dashed red circle) and the data.