It's relatively straightforward.
But perhaps you'd like to calculate this yourself?
First, let's find out the radius of the orbit.
You want to take the force of gravity between two bodies of masses equal to those of Earth's and Saturn's respectively, and compare that force to the one needed to keep the "moon" in a nice circular orbit(for simplicity's sake, and a good approximation anyway) - that is: centripetal force.
You end up with Fg=Fc
Where
Fg=GmM/r2
Fc=mrω2
and
the angular velocity ω=2∏/T
where T is one day(or 86400s)
So:
GM/r2=r4∏2/T2
GMT2=r34∏2
finally
r=(GMT2/4∏2)1/3
I'll let you plug in all the numbers.(remember to use T in seconds)
With that ready, let's see what size will the Saturn's disc appear on the sky:
2R/r=θ
where 2R is Saturn's diameter, r is the distance we've just calculated, and θ is the angular size(in radians) it'll have.
Now we know how big it is on the sky. How fast does it move across it then?
It goes a full circle in 1day, so its apparent angular velocity on the sky is:
ε=2∏/T
with that velocity, it obscures any point in the sky for:
t=θ/ε
seconds.
Now, at the distance of 10AU(Saturn's orbit) from the Sun, the Sun's disc is 1/100th of the half a degree in angular size we see on Earth. So let's just treat it as a point-like source of light that spends the above calculated t time obscured by Saturn's disc. And that's your eclipse duration.
Of course, that'd only work for the "moon"'s orbit perfectly aligned with that of Saturn's around the Sun. Should it be inclined, the eclipses' periods will change.
If the "moon"'s orbit inclination is higher than θ, then there will be times in the ~30 year long, well, year, when there are no eclipses, and times when the eclipses are shorter than the t we calculated, varying in a sinusoidal fashion from 0 to t.
In such case the eclipses would last full t time precisely twice in a year.
If the inclination is less than θ, the eclipse times will similarly vary between t and some value x, where t>x>0.
Yeah, so I did go ahead and plugged some numbers in, just to check if the results are roughly sensible, and I got:
r=200000km {~1/2th the distance from Earth to Moon and some 50000 km above the Satrun's Roche limit}
θ=0.6 rad {which is roughly 33 degrees, or 1/6th of the sky}
ε=7*10-5 rad/s
t=~8500s {2.3 hours}
An orbit inclined as much as, or more, than 33 degrees for a large moon seems unlikely, so the actual eclipse times would most likely never go below two hours for modestly inclined orbits.