Editing: I’m working this one out on paper to make it clearer. I think this answer as it stands is in the right direction but has two flaws.
To me there seems to be an obvious symmetry here - the hard part is just figuring out exactly what the symmetry is! First I thought about the target circle being a reflection of the 1-point circle (A) but I didn't get anywhere.
However, considering the possible space of points covered, I found an intuitive solution I think. Consider the ‘shadow’ of the target circle - the region of the plane where a line passing through the middle circle must hit the target circle. Now consider the areas swept out by possible lines in either situation. With BC, the whole plane can be covered. With AB, I think again the whole plane can be covered (except maybe a 0-measure set the vertical line tangent to both circles A and B). So then (I'll update this assumption in the morning if someone reminds me) I'm PRETTY sure that the shadow for AB and the shadow for BC is the same (because both lines pass through B I think?) so looking at the shadow divided by swept area we find that the two probabilities are equal. I guess infinitesimally less for BC.
Okay, I’m awake and wrote this up:
This solution is based on thinking of the circles as being on the plane. First, let's name the circle A (which has the singleton point). B (which has two points), and T for target (the one the lines hit). Ultimately, we will equate the probability of a line hitting T with the fraction of the plane that T occludes. More precisely I think: we are considering the plane as covered by lines. The 'range' of B would be the entire plane: obviously, for any point X on the plane we can pick a line that passes through that point X and two points on B (B and C I believe in the question). The 'shadow' cast by T is the region of the plane which cannot be reached by such a line except by passing through T. If B were emitting (non bending) rays of light in the directions prescribed by (line BC) and T were opaque, then we'd see the shadow clearly. Then, we take the probability of hitting T to be the area of the shadow divided by the area of the range.
Concretely, this is:

I just read Nuclear Hoagie's answer a second ago to make sure mine doesn't overlap, and I think this is where we part ways. There need not be a 1-1 correspondence between lines of B and lines of A, because we're normalizing. This obviates the concern over the fact that each line through B can be achieved in two ways (by swapping points B and C). It doesn't matter - the areas and division erase this factor of 2. We're not concerned with comparative counts, we're concerned with ratios of areas.
Similarly, A has a 'range' defined by the allowed lines: the change is that these lines must pass through point A on circle A and at least one point B on circle B, rather than two points on the same circle (as for circle B). However, it is intuitively clear that still the entire plane is in the range of A, except for the vertical line which is tangent to both circle A and circle B. So, the denominator of our probability is the same (because this single line of area-measure 0 doesn't make a difference). In this sense, I suppose we are essentially integrating without actually integrating - we're totting up infinitesimal areas and tossing out sets of measure 0.
Moreover, it is clear that ALMOST EVERY (and I mean this in a way similar to the measure-theoretic sense) line allowed on A also could be a line of B; it intersects circle B twice. Actually this may not be strictly true in terms of measure, but it doesn't really matter. We only care about the shadow. This means we can restrict our attention to the lines which hit A, B, and T.
First we observe that if a line is permitted on B and hits T, it's part of the shadow of T for light source B (which we described above). This means that if a line (like the bulk of the lines permitted on A) hits two points on circle B and then intersects T, it's part of the shadow for B. Of course, because it's permitted on A and intersects T, it also is part of the shadow for A. So then these shadows are starting to look very similar, except if there are lines that are allowed on A but NOT on B, which still hit T.
So to pause and recap here, we've established the probability for B and removed the concern over 1-1 correspondences by normalizing using area division. We've also established that, again NOT worrying about 1-1 correspondence or 'layers' of covering the plane, the denominator for the probability fraction for A is the same as that for B. So if we can then establish that the numerators (the shadows) are the same (up to differences of measure 0) then we know the two probabilities are the same.
There are a few exceptions to our previous discussion. These are the lines that start on A, hit only 1 point on B (as required), and go on to hit T. We can pretty easily say that these are only the two tangents which are tangent to all three circles. This is a finite set of measure-0 lines, which contributes nothing to the area of course. So the shadow size is also the same. Then dividing, we get the same probability.
So the answer is as suggested by the brute integration (which I was frankly never going to do myself): they're equal.
Edit: Dan raises the potential objection that this argument might seem to imply the probabilities remain equal when the red circle (A) is shifted to the right. I contend that my argument would no longer apply. The reasoning:
My original argument depends on the ratio of shadow to total possible area being equal for A and B. In the original problem, for both A and B, it is only possible to cover the plane with lines twice. That is, for any given direction or angle of line, we could get it two ways. For lines on B, we could get (for example) a line using B at the southwest and C at the northeast for 45 degrees. Or, we could switch B and C and get the exact same line. I established that almost every line allowed on A also passes through two points on B, which means we can pick two identical lines again. The tangents to B that hit A can likewise pass through two points on A so we can again pick two identical lines. So for lines allowed on A, we can cover (almost) the entire plane twice, just like B. The vertical tangent to A and B can never be reached, but that’s infinitesimally small as an area: the plane is covered twice by A or B, just the same. Remember, we’re ignoring T here.
So the denominator would be the same.
HOWEVER: when Dan poses this shifting of A, we lose the equivalency of the denominators. This is because as long as even a tiny stretch of the perimeter of A is contained within the ring of B, we suddenly re-cover the plane an uncountably infinite number of times. For every point of A inside B, we can pick a point on B to get a line in whatever direction we want. In fact. We can pick two such points! So then the sizes of the numerator and denominator get all out of whack and we can’t equate them or keep track of them at all. This means there’s no conclusion about any situation other than when A and B are tangent at exactly one point.