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In celestial mechanics, the specific relative angular momentum (often denoted h → {\displaystyle {\vec {h}}} or h {\displaystyle \mathbf {h} } ) of a body is the angular momentum of that body divided by its mass. In the case of two orbiting bodies it is the vector product of their relative position and relative linear momentum, divided by the mass of the…
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momentum specific displaystyle angular mathbf relative vector constant mass frac two second body times product position orbital time one equation
| Subject | Predicate | Object | Confidence | Src |
|---|---|---|---|---|
| Specific angular momentum | related to Proof of constancy in the two body case | Under | 0.60 | section |
| Specific angular momentum | related to Proof of constancy in the two body case | The | 0.60 | section |
| Specific angular momentum | related to Proof of constancy in the two body case | Each | 0.60 | section |
| Specific angular momentum | related to Proof of constancy in the two body case | No | 0.60 | section |
| Specific angular momentum | see also | Specific | 0.60 | section |
| Specific angular momentum | see also | Classical | 0.60 | section |
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