For the spin, we have the Sun. That isn’t truly stationary but it’s close enough; pound a stake into the ground, wait for its shadow to get to its shortest, start a stopwatch, the next day wait for the shadow to get to its shortest, stop the stopwatch and you’ve measured how fast the planet spins. (That’s the synodic day which is slightly different from the sidereal day, but you’re five so let’s keep it simple. :D)
For the orbit – imagine you’re looking at a billboard, and then you take six steps to the left and look at it again. It’s not a big difference, but you’re seeing the billboard from a slightly different angle now and if you took some careful measurements, you could tell that you’d moved. Conversely, if you know how far you’ve moved and take some measurements on the billboard, you could determine how far away the billboard is. A Greek philosopher whose name isn’t coming to me took some readings of the Moon’s location, and arranged for a colleague in another city to take readings on the same nights, and then they did some geometry and figured out how far away the Moon was. (They did damned well – less than 10% off the figure we believe today.)
Once they knew how far the Moon is…they figured out that when we’re seeing a half-moon, that must mean that Earth, the Moon and the Sun are at a 90-degree angle. If you know the 90, the angle from Earth to the Sun, and the distance from Earth to the Moon, you have enough to totally solve that triangle and now you know how far Earth is from the Sun. Multiply that by 2pi and you know the circumference of our orbit; divide that distance by 365.25 days and you have our orbital velocity.
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