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Velocity of the particle m with respect to the origin O can be resolved into components parallel to (v∥) and perpendicular to (v⊥) the radius vector r. The angular momentum of m is proportional to the perpendicular component v⊥ of the velocity, or equivalently, to the perpendicular distance r⊥ from the origin.

角運動量の物理学回転運動を支配する基本原理

角運動量慣性モーメントトルク角運動量保存の法則
続きを読む →
Velocity of the particle m with respect to the origin O can be resolved into components parallel to (v∥) and perpendicular to (v⊥) the radius vector r. The angular momentum of m is proportional to the perpendicular component v⊥ of the velocity, or equivalently, to the perpendicular distance r⊥ from the origin.

角運動量の物理学回転運動を支配する基本原理と保存則

角運動量慣性モーメントトルク角運動量保存の法則
続きを読む →