Newton connected the dots between Kepler’s third law (about planetary motion) and the concept of gravity. He realized
Real-World Analogy: Think of gravity as an invisible string tied between a planet and a satellite, constantly pulling them together. Without this string, the satellite would fly off!
Imagine a cannon on a really tall mountain
Scenario A: The cannon fires its ball horizontally. Because Earth isn’t flat (it’s a big round ball), the cannonball doesn’t just drop straight down. It travels a bit before being pulled down by gravity. Like throwing a stone!
Scenario B: If we shoot the cannonball even faster, it'll go even further before dropping.
Scenario C: At a SUPER high speed, the cannonball will go around Earth without touching it. It's now an orbiting satellite!
Real-World Analogy: Think of swinging a ball on a string around you. The string keeps the ball from flying off. Similarly, gravity is the "invisible string" keeping satellites in orbit!
The gravitational pull (FG
) acts as the centripetal force (FC
) that keeps the satellite in its orbit.
They gave this relationship
FC = FG = mω2 r = GMEm/r2
But, because math is magic, some symbols cancel out, and we get
ω2 r = GME/r2
Fun Fact: Here ω
is the satellite’s orbital speed, ME
is Earth's mass, and m
is the satellite's mass. And, G
is a universal gravitational constant.
Dive deeper and gain exclusive access to premium files of Physics SL. Subscribe now and get closer to that 45 🌟
Newton connected the dots between Kepler’s third law (about planetary motion) and the concept of gravity. He realized
Real-World Analogy: Think of gravity as an invisible string tied between a planet and a satellite, constantly pulling them together. Without this string, the satellite would fly off!
Imagine a cannon on a really tall mountain
Scenario A: The cannon fires its ball horizontally. Because Earth isn’t flat (it’s a big round ball), the cannonball doesn’t just drop straight down. It travels a bit before being pulled down by gravity. Like throwing a stone!
Scenario B: If we shoot the cannonball even faster, it'll go even further before dropping.
Scenario C: At a SUPER high speed, the cannonball will go around Earth without touching it. It's now an orbiting satellite!
Real-World Analogy: Think of swinging a ball on a string around you. The string keeps the ball from flying off. Similarly, gravity is the "invisible string" keeping satellites in orbit!
The gravitational pull (FG
) acts as the centripetal force (FC
) that keeps the satellite in its orbit.
They gave this relationship
FC = FG = mω2 r = GMEm/r2
But, because math is magic, some symbols cancel out, and we get
ω2 r = GME/r2
Fun Fact: Here ω
is the satellite’s orbital speed, ME
is Earth's mass, and m
is the satellite's mass. And, G
is a universal gravitational constant.
Dive deeper and gain exclusive access to premium files of Physics SL. Subscribe now and get closer to that 45 🌟
AI Assist
Expand