Find new point of tangency on circular arc having second point which is known but unknown center 
The more I try to figure this one out, the more I realize I don't recall everything I need to attack this problem, despite doing well in geometry classes (about 15 years ago). It appears to be a problem in two parts.
A line, $\overline{bf}$, is tangent to arc segment $\overline{ab}$ with center $c$, and fixed at point $a$. Line $\overline{bf}$ is rotated by $6$ degrees to become line $\overline{df}$, causing the arc radius to decrease to $R$, but the arc remains fixed at point $a$ and tangent to the original arc. The center $c$ moves to point $e$ due to the decrease in radius, but remains coincident with line $\overline{ag}$. Line $\overline{fg}$ has fixed length $W$ and is equal to the starting radius of arc segment $\overline{ab}$, but not equal to the finishing radius of arc segment $\overline{ad}$.
I need to find (a) the new radius $R$ and (b) the values of $dx$ and $dy$ for the tangent point ($x$ and $y$ distances to the new point of tangency). An algebraic form solution would be appreciated. Thanks very much in advance.
 A: Your drawing is very... unusual. What's wrong with capital letters? 
Note that $\angle dea=90^\circ-6^\circ=84^\circ$. 
$$\overline{bc} = dx+R\sin \angle dea$$
$$\overline{ga}=\overline{df}\cos \angle bfd-R\cos \angle dea + R\tag{2} $$
This leads to:
$$\overline{df} \sin 6^\circ+R\sin 84^\circ=W\tag{3}$$
$$\overline{df}\cos 6^\circ-R\cos 84^\circ + R=W+H\tag{4} $$
This linear system of two equations, (3) and (4), has two unknows, $\overline{df}$ and $R$, and can be easily solved in terms of $W$ and $H$.
The rest is easy:
$$dx=\overline{df}\sin 6^\circ$$
$$dy=\overline{df}\cos 6^\circ-H$$
A: Calling the small circle $C$ and the tangent slanted line $L$
$$
C \to x^2+(y-y_c)^2=r^2\\
L \to y = f_y+m(x-f_x)
$$
with $m = \tan\theta_0, f = (f_x,f_y)$
the tangency between $L$ and $C$ is obtained as follows
Substituting $y$ from $L$ into $C$ we have
$$
(m (x-f_x)+f_y-y_c)^2-r^2+x^2 = 0
$$
solving for $x$ we have
$$
x=\frac{\pm\sqrt{\left(m^2+1\right) r^2-(y_c+f_x m-f_y)^2}+m (y_c+f_x m-f_y)}{m^2+1}
$$
but tangency imposes
$$
\sqrt{\left(m^2+1\right) r^2-(y_c+f_x m-f_y)^2}=0
$$
or solving for $y_c$
$$
y_c = f_y-m f_x\pm r\sqrt{m^2+1}
$$
taking the condition that in $C$ we have $0^2+(R-y_c)^2 = r^2$ and solving
$$
y_c = f_y-m f_x\pm r\sqrt{m^2+1}\\
(R-y_c)^2 = r^2\\                                               
$$
we obtain $r, y_c$. Now the tangency point $d$ is obtained knowing that 
$$
t_0 = \sqrt{||f-e||^2-r^2}
$$
and then
$$
p = f + t_0(\cos\theta_0,\sin\theta_0)
$$
etc,
Attached a plot for the realization with
$$
f = (-1,2)\\
\theta_0 = 84^{\circ}\\
R = 1
$$

A: You can compute all of these values directly. I’m going to rotate the diagram so that $c$ is at the origin, $a$ is at $(W,0)$, $b$ is at $(0,W)$ and $f$ is at $(-H,W)$.  
The center of a circle lies on one of the angle bisectors of a pair of its tangents. This can be used to find the new center $e$ as follows: Using homogeneous coordinates, the tangent line at $a$ is $\mathbf l = [1:0:-W]$ and the rotated line through $f$ is $\mathbf m = [\sin\theta:\cos\theta:H\sin\theta-W\cos\theta]$. Both of these representations have unit normals, so the angle bisectors of the two lines are simply the sum and difference of these vectors. For this problem, the appropriate bisector to use is the difference. Its $x$-intercept is the new center $e = (\mathbf l-\mathbf m)\times[0:1:0]$, which is easily computed to be $$x_e = {W(1-\cos\theta)+H\sin\theta \over 1-\sin\theta}.$$ This is the amount by which the original circle center is offset toward $a$. The new radius is then simply $r = W-x_e$ and the point $d = e+r(\sin\theta,\cos\theta)$. Finally, its offset from $b$ is $e-b+r(\sin\theta,\cos\theta)$. I’ll leave expanding this to you.
