Video Experimental Relacionado
Updated: Mar 26, 2026

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
8.6K
El deslizamiento lento periódico desencadena terremotos de la zona megatrust en el noreste de Japón
Naoki Uchida1, Takeshi Iinuma2, Robert M Nadeau3
1Graduate School of Science and International Research Institute of Disaster Science, Tohoku University, 6-6, Aramaki-aza-aoba, Aoba-ku, Sendai 980-8578, Japan.
Resumen
Eventos casi periódicos de deslizamiento lento en Japón
Área de la Ciencia:
- La geofísica
- Tectónica
- Sismología
Sus antecedentes:
- Las fallas del límite de la placa se adaptan al movimiento relativo a través del deslizamiento sísmico y asísmico.
- En el noreste de Japón, el deslizamiento sísmico incluye el deslizamiento posterior y el deslizamiento constante en áreas de empuje de subducción no acopladas.
Objetivo del estudio:
- Para informar sobre un comportamiento de deslizamiento lento cuasi-periódico recién identificado en la zona megathrust.
- Para investigar la relación entre los eventos de deslizamiento lento y los grandes terremotos.
Principales métodos:
- Análisis de datos geológicos para identificar eventos de deslizamiento lento.
- Correlación del tiempo del evento de deslizamiento lento con la actividad sísmica.
Principales resultados:
- Se identificó un comportamiento de deslizamiento lento cuasi periódico generalizado y no reconocido previamente en la zona de megatrust.
- Los eventos de deslizamiento lento se repiten cada 1 a 6 años.
- Estos eventos a menudo coinciden con o preceden a grupos de grandes terremotos (M ≥ 5), incluido el terremoto de Tohoku-oki M 9 de 2011.
Conclusiones:
- Es probable que los eventos periódicos de deslizamiento lento causen cambios periódicos de estrés.
- Los eventos de deslizamiento lento modulan el tiempo de los terremotos más grandes.
- La periodicidad del deslizamiento lento puede mejorar el pronóstico de terremotos dependientes del tiempo.
Videos de Conceptos Relacionados
Fault Types
483
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...
483
Forced Oscillations
8.2K
When an oscillator is forced with a periodic driving force, the motion may seem chaotic. The motions of such oscillators are known as transients. After the transients die out, the oscillator reaches a steady state, where the motion is periodic, and the displacement is determined.
8.2K
Atomic Nuclei: Larmor Precession Frequency
3.6K
The earth's gravitational field produces a 'twisting force' perpendicular to the angular momentum of a spinning mass (such as a spinning top) that causes the mass to 'wobble' around the gravitational field axis in a phenomenon called precession. Similarly, the magnetic moment (μ) of a spinning nucleus precesses due to an external magnetic field directed along the z-axis. The precession of the magnetic moment vector about the magnetic field is called Larmor precession,...
3.6K
Atomic Nuclei: Types of Nuclear Relaxation
1.2K
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...
1.2K
Elastic Strain Energy for Shearing Stresses
595
As discussed in previous lessons, strain energy in a material is the energy stored when it is elastically deformed, a concept crucial in materials science and mechanical engineering. This energy results from the internal work done against the cohesive forces within the material. When a material undergoes shearing stress and corresponding shearing strain, the strain energy density, which is the energy stored per unit volume, is calculated. Within the elastic limit, where the stress is...
595
Magnetostatic Boundary Conditions
1.8K
An electric field suffers a discontinuity at a surface charge. Similarly, a magnetic field is discontinuous at a surface current. The perpendicular component of a magnetic field is continuous across the interface of two magnetic mediums. In contrast, its parallel component, perpendicular to the current, is discontinuous by the amount equal to the product of the vacuum permeability and the surface current. Like the scalar potential in electrostatics, the vector potential is also continuous...
1.8K

