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Concept module
Escape Velocity
Launch outward from one bounded gravity source and see how source mass, launch radius, and total specific energy decide whether the object escapes or eventually returns.
Interactive lab
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Progress
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Stable links
Why it behaves this way
Explanation
Escape velocity is the minimum outward launch speed from one chosen radius that makes the total specific energy reach zero. Above that threshold, gravity still pulls inward and slows the launch, but there is no finite turnaround radius. Below it, even a very high outward trip is still bound and eventually returns.
This bounded lab keeps one source mass, one launch radius, one speed factor, one live radial path, and the linked radius, speed-threshold, and specific-energy graphs on the same state. The local circular-speed comparison stays visible too, so going far away is not confused with escape or with circular orbit balance.
Key ideas
Frozen walkthrough
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View plansFor the current source mass and launch radius, what outward launch speed makes the total specific energy exactly zero?
4 kg
1.6 m
1. Set the threshold condition
2. Solve for the threshold speed
3. Compute the live value
Escape speed
Escape-threshold checkpoint
Make a prediction before you reveal the next step.
Check your reasoning against the live bench.
Common misconception
If a launch gets far enough from the source, it has escaped, and escape means gravity is basically gone.
Distance alone does not decide escape. The deciding quantity is the sign of E/m. Zero or positive total specific energy means there is no finite turnaround radius; negative total specific energy means the launch is still bound.
Gravity does not vanish after escape. It keeps acting and keeps reducing the speed. The difference is that the object never has to reverse direction.
Quick test
Reasoning
Question 1 of 4
A launch begins faster than the local circular-speed comparison but still below the escape speed from the same radius. What must be true in this lab?
Use the live bench to test the result before moving on.
Accessibility
The simulation shows one source mass on the left side of a compact radial launch axis, a launched mass moving outward or inward along that axis, and optional overlays for the launch marker, finite turnaround marker, current velocity vector, inward gravity vector, and visited trajectory trail.
Changing source mass, launch radius, or speed factor updates the same trajectory, readout card, and linked graphs together. Compare mode overlays a second launch on a separate dashed track instead of switching to a different model.
The displayed units use a bounded one-source gravity model with G = 1. The stage has a finite maximum visible radius, and bound launches whose turnaround sits beyond that view are labeled explicitly rather than being faked into the visible window.
Graph summary
The radius-history graph compares the live radius with the starting launch radius over the same time window. Hovering or scrubbing the graph previews the same instant on the launch stage.
The speed-thresholds graph compares the live speed with the local escape-speed and circular-speed benchmarks, and the specific-energy graph shows the live kinetic, potential, and total specific energies together with the zero-energy threshold.
Keep the gravity launch story moving
Keep this idea moving
Open the next concept, route, or track only when you want the current model to widen into a larger branch.
Kepler's Third Law and Orbital Periods
Compare circular orbits around one source mass and see why larger orbits take longer: the path is longer, the circular speed is lower, and the same live model makes the period law visible without hiding the gravity-speed link.
Circular Orbits and Orbital Speed
See why a circular orbit needs the right sideways speed, how gravity supplies the centripetal acceleration, and how source mass and radius together set orbital speed and period on one bounded live model.
Gravitational Potential and Potential Energy
See one source mass create a negative potential well, compare how potential and potential energy change with distance, and connect the downhill slope of phi to the gravitational field on the same live model.