I want to mention something further about finding the satellite's acceleration. You used the form of the centripetal acceleration equation involving the angular frequency of the orbit to get
a_c = (2·pi/21600 sec)^2 · 1.676·10^7 m = 1.42 m/(sec^2) .
You could also have used the version involving the linear velocity on the orbit:
v = C/T = (2·pi·r)/T or sqrt[G·(Me)/r] = 4875 m/sec , and
a_c = (v^2)/r ,
which is otherwise equivalent to the form you used.
You could also use the gravitational force equation, to find
F_g = G·Me·m/(r^2) = F_c = m·a_c ,
m being the satellite's mass [this equation, BTW, also gives us the "weight" of the spacecraft at this altitude above the Earth's surface -- more on this presently] , which leads to
a_c = G·Me/(r^2)
= [6.67·10^-11 N·(m^2)/(kg^2)] · (5.98·10^24 kg) / [(1.676·10^7 m)^2]
= 1.42 m/(sec^2) .
Since m does not appear in this result, this shows that any small satellite experiences the same acceleration on this orbit.
There is yet another approach using comparison ratios. The gravitational force between Earth and the satellite obeys the same relation at any radius from the Earth's surface outward. So the acceleration the satellite would experience at the Earth's surface would be
a' = G · Me / (R^2) ,
where R is the Earth's radius. You may recognize this expression as giving g , the acceleration of gravity at the Earth's surface. We can now compare this to the acceleration in the satellite's orbit:
a_c / g = [ G·Me/(r^2) ] / [ G·Me/(R^2) ] = (R/r)^2 .
In this method, we don't even need to know the value of G or the Earth's mass (much less the satellite's mass, m), since the constants all cancel out in the comparison. So we find
a_c = [ (R/r)^2 ] · g = [ (6378 km / 16,758 km)^2 ] · (9.81 m/sec^2)
= (0.3806^2) · (9.81 m/sec^2) = 1.42 m/(sec^2) .
This is another way of saying that the satellite in orbit weighs 0.3806^2 = 0.145 (about 1/7) of what it weighs on Earth.
Many roads leading to the same place (because they're all really basically equivalent)...