I’ve worked this out - with a few simplifying assumptions. As I understand it, we’re assuming that this rift in the earth occurred magically, leaving two hemispheres (trying to) continue rotating about one another. Would the gravitational attraction provide the necessary centripetal (no, I don’t mean “centrifugal”) force, or not?
To greatly simplify my life, I’m going to assume that the earth is a sphere of uniform density. This is clearly not true, but I’m going to run with it anyway. I’m also going to assume that the rotational period of the earth is precisely 24 hours (it’s not), and I’m going to ignore the fact that the earth is rotating around the sun.
Mass of earth, m = 5.97x10[sup]24[/sup] kg.
Angular velocity, [sym]W[/sym] = 2[sym]p[/sym] radians/day = 7.27x10[sup]-5[/sup] rad/sec
Radius of earth, R = 6.378x10[sup]5[/sup] m
When the two halves split, they’ll each have a mass of m[sub]H[/sub] = 2.99x10[sup]24[/sup] kg. We also need to know the center of mass of each half. This is where the assumption of uniform density comes in handy.
This page is kind enough to derive the center of mass of a uniform hemisphere for us - it’s a distance of (3/8)R out from the center of the original sphere. What this means is that once the split occurs, we can treat it as two bodies of mass m[sub]H[/sub] a distance of (3/4)R apart. Call this separation D[sub]H[/sub] = 0.75R = 4.78x10[sup]5[/sup] m. Let R[sub]H[/sub], half of that, be the distance of each body from the center of rotation. R[sub]H[/sub] = 2.39x10[sup]5[/sup] m.
What is the magnitude of the gravitational attraction between the two halves? This is given by:
G m[sub]H[/sub][sup]2[/sup]
F[sub]G[/sub] = ----- = 2.6x10[sup]27[/sup] N
D[sub]H[/sub][sup]2[/sup]
where G, the universal gravitational constant, has a value of 6.673x10[sup]-11[/sup] N m[sup]2[/sup] kg[sup]-2[/sup].
OK, great. Is that sufficient to act as a centripetal force to keep a hemisphere orbiting about the original center of the earth? The force required to do that is given by:
m[sub]H[/sub]([sym]W[/sym]R[sub]H[/sub])[sup]2[/sup]
F[sub]C[/sub] = -------- = m[sub]H[/sub][sym]W[/sym][sup]2[/sup]R[sub]H[/sub] = 3.78x10[sup]21[/sup] kg m/s[sup]2[/sup] = 3.78x10[sup]21[/sup] N
R[sub]H[/sub]
The gravitational attraction is about a million times stronger than that, so it will easily be enough to hold the two halves together.
How fast would the earth need to be spinning so that it would fly apart under these conditions? We need F[sub]C[/sub] > F[sub]G[/sub], or
Gm[sub]H[/sub]
[sym]W[/sym][sup]2[/sup] > ------ = 3.65x10[sup]-3[/sup] s[sup]-2[/sup]
4R[sub]H[/sub][sup]3[/sup]
which is [sym]W[/sym] = 6.04x10[sup]-2[/sup] radians/sec, or about 830 revolutions per day.
I think it’s safe to say that Chronos is quite right - if the earth were spinning that quickly, we’d have all sorts of problems to worry about. In fact, I’d say that if there were that much angular momentum floating around, the earth would never have formed in the first place, since I believe planetary accretion is predominantly gravitaional forces slowly overcoming rotational ones.