A New Theoretical Framework for the Helical Motion of Celestial Bodies in Relation to the Einstein–Rosen Wormhole Model in the Universe

Looking at our Moon, it orbits the Earth, which orbits the Sun. If an observer views the Moon and Earth together, they see both moving around the Sun. The Earth’s path is a closed curve, returning after a year. In contrast, since the Moon orbits the Earth while also orbiting the Sun, it follows a simple helical path.

Now, if we consider the motion of the Sun, orbiting the supermassive black hole at the centre of the Milky Way, the Earth follows the Sun in its path. When an observer considers the Earth and Sun within the galaxy, they can show that the Earth has a helical motion. This gives a general rule: whenever a celestial object, such as a moon, planet, star, or galaxy, has ‘n’ orbits, it can be shown to have n-1 helical paths.

Since the Milky Way belongs to a cluster or even a supercluster, it’s clear that, in addition to its closed curve motion, the Milky Way can have more helical paths. For example, within the Milky Way, a moon like ours has at least two helical motions: one orbiting the Earth, another orbiting the Sun, and a third around the galactic centre. Similarly, the Earth has at least one helical motion in the Milky Way. Because galaxies and clusters move in higher-level structures, galaxies must also possess helical motion.

Based on the principle of helical motion in the cosmos, one might conceptualize the central axis of a helical motion as analogous to an Einstein-Rosen bridge. Simply put, an axis passing through the helical motion of celestial objects can be defined as the Einstein-Rosen wormhole.