Gravitational fields and orbital motion
| English | 中文 | Pinyin |
|---|---|---|
| gravitational field/ˌɡrævɪˈteɪʃənl fiːld/ | 引力场 | yǐn lì chǎng |
| centripetal force/senˈtrɪpɪtl fɔːs/ | 向心力 | xiàng xīn lì |
What would explain this observation?
- An orbiting satellite is continuously falling while moving sideways. Being in orbit does not require gravity to vanish.
- Start with a prediction. State the quantities or features you would compare, then decide what evidence could distinguish two explanations.
Build the model
- Gravitational field 引力场 strength is force per unit mass. A gravitational force can provide the centripetal force 向心力 for a circular orbit. Field and potential describe different quantities.
- gravitational field: A description of gravitational force per unit mass; centripetal force: Net force toward the centre of a curved path.
What direction is the net force in uniform circular motion?
For a point mass or outside a spherical mass, field strength follows an inverse-square distance dependence. Use distance from the centre, not height above the surface alone.
Match each technical term to its precise meaning.
Use the definitions to distinguish related quantities and processes.
Choose evidence that can test it
- For a point mass or outside a spherical mass, field strength follows an inverse-square distance dependence. Use distance from the centre, not height above the surface alone.
- State the circular-orbit approximation and ignore atmospheric drag only when justified. Draw the force toward the central body and velocity tangential to the orbit. Do not add an outward force merely because the path is circular.
Which two habits make the investigation or model in this case more defensible?
State the circular-orbit approximation and ignore atmospheric drag only when justified. Draw the force toward the central body and velocity tangential to the orbit. Do not add an outward force merely because the path is circular.
Work from known quantities
- State the known values and their units. Choose the relation because its assumptions fit this case, then rearrange before substitution.
- Known: field strength is 8 units at distance r from a spherical source. At 2r, g2/g1=(r/2r)²=1/4. g2=8/4=2 units. The gravitational force on a fixed test mass decreases in the same ratio.
Field strength is 18 units at r. Find it at 3r for an inverse-square field. Use the same sequence: known quantities → model → relation → substitution → unit and interpretation.
Field strength is 18 units at r. Find it at 3r for an inverse-square field.
The result is 2 . Known: field strength is 8 units at distance r from a spherical source. At 2r, g2/g1=(r/2r)²=1/4. g2=8/4=2 units. The gravitational force on a fixed test mass decreases in the same ratio.
Check the conclusion and its limits
- Weightlessness in an orbiting spacecraft means apparent weight is small in free fall, not that there is no gravitational field.
- Return to the original observation. Explain what the result supports, which conditions it assumes, and one way to test a competing explanation.
Gravity is zero everywhere a spacecraft experiences apparent weightlessness. This claim is false: Weightlessness in an orbiting spacecraft means apparent weight is small in free fall, not that there is no gravitational field.
Gravitational fields and orbital motion: For a point mass or outside a spherical mass, field strength follows an inverse-square distance dependence. Use distance from the centre, not height above the surface alone.
Gravity is zero everywhere a spacecraft experiences apparent weightlessness.
Weightlessness in an orbiting spacecraft means apparent weight is small in free fall, not that there is no gravitational field.
A description of gravitational force per unit mass: write the technical term.
gravitational field means A description of gravitational force per unit mass.