Gravitational Quadrupoles Archives - Time Travel, Quantum Entanglement and Quantum Computing https://stationarystates.com/tag/gravitational-quadrupoles/ Not only is the Universe stranger than we think, it is stranger than we can think...Hiesenberg Wed, 25 Jun 2025 17:04:33 +0000 en-US hourly 1 https://wordpress.org/?v=6.9.1 Why are there Gravitational Quadrupoles? https://stationarystates.com/general-relativity-and-cosmology/why-are-there-gravitational-quadrupoles/?utm_source=rss&utm_medium=rss&utm_campaign=why-are-there-gravitational-quadrupoles Thu, 19 Jun 2025 23:29:10 +0000 https://stationarystates.com/?p=945 Why Are There Gravitational Quadrupoles? 1. No Monopole Radiation A gravitational monopole would require changes in the total mass of a system. However, total mass is conserved in isolated systems, […]

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Why Are There Gravitational Quadrupoles?

1. No Monopole Radiation

A gravitational monopole would require changes in the total mass of a system.
However, total mass is conserved in isolated systems, so there is no time-varying monopole.
Therefore, no gravitational monopole radiation exists.

2. No Dipole Radiation

In electromagnetism, dipole radiation arises from oscillating positive and negative charges.
In gravity, only positive mass exists. So there’s no gravitational equivalent of charge separation.
Even when masses move, the dipole moment (i.e., the center of mass) of a closed system remains constant.
Thus, no gravitational dipole radiation occurs.

3. Quadrupole Is the First Non-Zero Radiating Term

Gravitational radiation results from time-varying asymmetric mass distributions.
This is captured by the quadrupole moment tensor:

    \[ Q_{ij} = \int \rho(\vec{r}) \left( r_i r_j - \frac{1}{3} \delta_{ij} r^2 \right) \, d^3r \]

When this quadrupole moment changes over time, it radiates gravitational waves.

Examples of Quadrupole Sources

  • Binary star systems (e.g., neutron star mergers)
  • Rotating dumbbell-shaped mass distributions
  • Asymmetric stellar collapses (supernovae)

These systems exhibit a time-varying quadrupole moment, which produces gravitational radiation.

Einstein’s Quadrupole Radiation Formula

The power P radiated in gravitational waves is given by:

    \[ P = \frac{G}{5c^5} \left\langle \dddot{Q}_{ij} \dddot{Q}^{ij} \right\rangle \]

This depends on the third time derivative of the quadrupole moment tensor,
showing how gravitational wave emission is tied to rapidly accelerating mass configurations.

Summary Table

Radiation Type Electromagnetism Gravity
Monopole Yes (oscillating charge) No (mass conserved)
Dipole Yes (charge separation) No (no negative mass)
Quadrupole Not required Yes (first allowed radiating term)

Visual Intuition

A perfectly symmetric spinning sphere doesn’t change its mass distribution and emits no gravitational radiation.
But a dumbbell-shaped system of two orbiting masses constantly changes its quadrupole moment,
producing gravitational waves — this is what LIGO and similar detectors are designed to observe.

 

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