Sluggish thermochemical basal mantle structures support their long-lived stability.
Zhidong Shi1,2, Ross N Mitchell1,2, Yang Li3,4
1State Key Laboratory of Lithospheric and Environmental Coevolution, Institute of Geology and Geophysics, Chinese Academy of Sciences, Beijing, 100029, China.
Nature Communications
|November 20, 2024
Summary
Numerical models reveal that large low shear-wave velocity provinces (LLSVPs) in the deep mantle likely formed from thermochemical structures. These ancient, slow-moving features explain geological observations over millions of years.
Area of Science:
- Geophysics
- Earth Sciences
- Mantle Dynamics
Background:
- Large low shear-wave velocity provinces (LLSVPs) are enigmatic, massive structures in Earth's deep mantle.
- Geological evidence suggests LLSVPs have been stable for at least 200 million years.
Purpose of the Study:
- To investigate the origin and long-term stability of LLSVPs.
- To model the formation of basal mantle structures resembling LLSVPs.
Main Methods:
- Numerical modeling of mantle convection incorporating plate-like behavior.
- Parameterization of models to match observed LLSVP characteristics.
Main Results:
- A Pacific-like downwelling girdle successfully generated two antipodal basal mantle structures similar to LLSVPs.
- Modeled thermochemical structures exhibited velocities approximately four times slower than the ambient mantle, consistent with long-term stability.
Conclusions:
- The sluggish, thermochemical nature of modeled basal mantle structures supports their ancient origin and stability.
- This provides a potential mechanism linking geological observations across hundreds of millions of years to modern LLSVPs.
Related Concept Videos
Nuclear Stability
18.6K
Protons and neutrons, collectively called nucleons, are packed together tightly in a nucleus. With a radius of about 10−15 meters, a nucleus is quite small compared to the radius of the entire atom, which is about 10−10 meters. Nuclei are extremely dense compared to bulk matter, averaging 1.8 × 1014 grams per cubic centimeter. If the earth’s density were equal to the average nuclear density, the earth’s radius would be only about 200 meters.
To hold positively charged protons together...
To hold positively charged protons together...
18.6K
Phase Transitions: Sublimation and Deposition
16.8K
Some solids can transition directly into the gaseous state, bypassing the liquid state, via a process known as sublimation. At room temperature and standard pressure, a piece of dry ice (solid CO2) sublimes, appearing to gradually disappear without ever forming any liquid. Snow and ice sublimate at temperatures below the melting point of water, a slow process that may be accelerated by winds and the reduced atmospheric pressures at high altitudes. When solid iodine is warmed, the solid sublimes...
16.8K
Atomic Nuclei: Types of Nuclear Relaxation
260
Nuclear relaxation restores the equilibrium population imbalance and can occur via spin–lattice or spin–spin mechanisms, which are first-order exponential decay processes.
In spin–lattice or longitudinal relaxation, the excited spins exchange energy with the surrounding lattice as they return to the lower energy level. Among several mechanisms that contribute to spin–lattice relaxation, magnetic dipolar interactions are significant. Here, the excited nucleus transfers...
In spin–lattice or longitudinal relaxation, the excited spins exchange energy with the surrounding lattice as they return to the lower energy level. Among several mechanisms that contribute to spin–lattice relaxation, magnetic dipolar interactions are significant. Here, the excited nucleus transfers...
260
Phase Transitions: Melting and Freezing
12.3K
Heating a crystalline solid increases the average energy of its atoms, molecules, or ions, and the solid gets hotter. At some point, the added energy becomes large enough to partially overcome the forces holding the molecules or ions of the solid in their fixed positions, and the solid begins the process of transitioning to the liquid state or melting. At this point, the temperature of the solid stops rising, despite the continual input of heat, and it remains constant until all of the solid is...
12.3K
Third Law of Thermodynamics
18.2K
A pure, perfectly crystalline solid possessing no kinetic energy (that is, at a temperature of absolute zero, 0 K) may be described by a single microstate, as its purity, perfect crystallinity,and complete lack of motion means there is but one possible location for each identical atom or molecule comprising the crystal (W = 1). According to the Boltzmann equation, the entropy of this system is zero.
18.2K
Thermal Sigmatropic Reactions: Overview
2.1K
Sigmatropic rearrangements are a class of pericyclic reactions in which a σ bond migrates from one part of a π system to another. These are intramolecular rearrangements where the total number of σ and π bonds remain unchanged.
Sigmatropic shifts are classified based on an order term [i, j ], where i and j indicate the number of atoms across which each end of the σ bond migrates. Below are examples of a [3,3] sigmatropic shift in...
Sigmatropic shifts are classified based on an order term [i, j ], where i and j indicate the number of atoms across which each end of the σ bond migrates. Below are examples of a [3,3] sigmatropic shift in...
2.1K


