Using pythagoras you can find the length (x) of the opening in the shell:
(x/2)² + (r/3)² = r²
x = (4/3)sqrt[2] r
Since the marble was performing circular motion, it initially leaves the shell with a path that is tangent to the surface of the shell. In other words, it becomes a projectile with an angle A to the horizontal. Since its path is tangent to the circle, A=90-B, where B is the angle the radius makes with the point at the edge of the opening.
Basic trigonometry should give you:
cosB = (r/3)/r = 1/3
sinB = (x/2)/r = {[(4/3)sqrt[2] r]/2}/r = (2/3)sqrt[2]
(Hopefully this helped you understand what B is!)
The equation for the range of a projectile is:
R = [u² sin(2A)]/g, where u is the initial velocity of the projectile and NOT the initial velocity of the marble.
We know that R=x and that sin(2A) = 2sinAcosA = 2cosBsinB = 2(1/3)(2/3)sqrt[2] = (4/9)sqrt[2]. Then:
R = [u² sin(2A)]/g = u²(4/9g)sqrt[2]
(4/3)sqrt[2] r = u²(4/9g)sqrt[2]
r = u²(1/3g) => u²=3rg.
To avoid confusion, I'll replace u with U: U²=3rg.
Now, at the starting position:
KE = 0.5mv² = 0.5mu²
PE = 0
And at the tip of the opening:
KE = 0.5mv² = 0.5mU²
PE = mgh = mg(r+r/3) = (4/3)mrg
Conservation of energy gives:
0.5mu² = 0.5mU² + (4/3)mrg
u² = U² + (8/3)rg
u² = 3rg + (8/3)rg [since]
u² = (17/3)rg
This is the speed the marble should have to DIRECTLY land at the other end of the opening. So any speed greater than this would cause the marble to miss the opening and leave the circle, i.e.
u² > (17/3)rg
as required.