Related Experiment Video
Updated: Sep 29, 2025

06:55
Kinematic History of a Salient-recess Junction Explored through a Combined Approach of Field Data and Analog Sandbox Modeling
Published on: August 5, 2016
8.3K
Arc and forearc rifting in the Tyrrhenian subduction system
M Corradino1, A Balazs2, C Faccenna3,4
1Department of Earth and Marine Sciences, University of Palermo, Via Archirafi, 22, 90123, Palermo, Italy.
Scientific Reports
|March 19, 2022
Summary
Forearc and backarc evolution are linked through arc-rifting, driven by fluids and melts. This process formed a backarc basin and influenced subsequent forearc rifting in the Tyrrhenian subduction system.
Area of Science:
- Geology
- Geophysics
- Tectonics
Background:
- Forearc and backarc domains are typically studied independently due to their separation by volcanic arcs.
- The Tyrrhenian subduction system provides a unique setting to investigate the interplay between these domains.
Purpose of the Study:
- To analyze the spatial and temporal relationships between forearc and backarc evolution.
- To understand the mechanisms driving arc-rifting and basin formation in a subduction zone.
Main Methods:
- Analysis of seismic profiles.
- Numerical modeling of tectonic processes.
Main Results:
- Arc-rifting during the Pliocene, involving the Marsili volcano, led to the formation of an oceanic backarc basin approximately 1.8 million years ago.
- A new volcanic arc formed around 1 million years ago in the forearc domain, initiating forearc-rifting.
- Fluids and melts were identified as key factors weakening the volcanic arc and driving arc-rifting and backarc basin development.
Conclusions:
- The study demonstrates a direct link between volcanic arc weakening, arc-rifting, and backarc basin formation.
- Slab rollback influenced volcanism migration, leading to forearc-rifting controlled by fluids from the downgoing plate.
Related Concept Videos
Fault Types
135
When analyzing a single line-to-ground fault from phase A to ground at a three-phase bus, it is important to consider the fault impedance. This impedance is zero for a bolted fault, equal to the arc impedance for an arcing fault, and represents the total fault impedance for a transmission-line insulator flashover. To derive sequence and phase currents, fault conditions are translated from the phase domain to the sequence domain.
For line-to-line faults occurring between phases B and C, the...
For line-to-line faults occurring between phases B and C, the...
135
Node Analysis for AC Circuits
387
Consider an angioplasty system featuring a catheter equipped with a turbine, a critical tool for removing plaque deposits from coronary arteries. This intricate medical device operates using a circuit model reminiscent of a dual-node RLC circuit powered by a current-controlled voltage source.
To unravel the complexities of this system, nodal analysis is employed, a powerful technique founded on Kirchhoff's current law (KCL), which remains valid for phasors. AC circuits can effectively be...
To unravel the complexities of this system, nodal analysis is employed, a powerful technique founded on Kirchhoff's current law (KCL), which remains valid for phasors. AC circuits can effectively be...
387
Irrotational Flow
597
Irrotational flow is characterized by fluid motion where particles do not rotate around their axes, resulting in zero vorticity. For a flow to be irrotational, the curl of the velocity field must be zero. This imposes specific conditions on velocity gradients. For instance, to maintain zero rotation about the z-axis, the gradient condition:
597
Ionic Radii
29.9K
Ionic radius is the measure used to describe the size of an ion. A cation always has fewer electrons and the same number of protons as the parent atom; it is smaller than the atom from which it is derived. For example, the covalent radius of an aluminum atom (1s22s22p63s23p1) is 118 pm, whereas the ionic radius of an Al3+ (1s22s22p6) is 68 pm. As electrons are removed from the outer valence shell, the remaining core electrons occupying smaller shells experience a greater effective nuclear...
29.9K
Membrane Asymmetry Regulating Transporters
5.1K
Enzymes like flippase, floppase, and scramblase transfer phospholipids from one layer to another in the membrane, thereby affecting membrane asymmetry.
Flippase
Eukaryotic flippases are type-IV P-type ATPases or P4-ATPases belonging to P-type ATPase family proteins that are membrane-bound pumps involved in the ATP-mediated transport of ions and molecules across the membrane. Flippases flip specific phospholipids from the outer to the inner leaflet of a membrane. All P4-ATPases have one...
Flippase
Eukaryotic flippases are type-IV P-type ATPases or P4-ATPases belonging to P-type ATPase family proteins that are membrane-bound pumps involved in the ATP-mediated transport of ions and molecules across the membrane. Flippases flip specific phospholipids from the outer to the inner leaflet of a membrane. All P4-ATPases have one...
5.1K
Coriolis Force
4.4K
An accelerating particle experiences a force equal to the mass multiplied by the acceleration in an inertial frame of reference. Consider a particle in a non-inertial frame of reference, such as a sliding ball on a rotating table. The acceleration of the ball in this rotating reference frame is different than in the intertial frame, which modifies its equation of motion. The fictitious forces acting additionally on a rotating frame of reference alter Newton's Second Law expression.
4.4K

