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Bistable systems are hysteretic, that is, their behavior depends on the history of the input.
There are four major groups of hysteretic dampers used for the purpose, namely:
Parameters , and control the size and shape of the hysteretic loop.
A circuit that implements this form of hysteretic switching is known as a Schmitt trigger.
Hysteretic systems have two important properties.
For hysteretic materials such as ferromagnets and superconductors, the work needed also depends on how the magnetic field is created.
The relation between the sensor's electrical resistance and sensor matric potential is hysteretic.
In general, self-heating can turn a resistor into a nonlinear and hysteretic circuit element.
The restoring force can be decomposed into an elastic and a hysteretic part as follows:
The , and are defined as linearly-increasing functions of absorbed hysteretic energy :
The Bouc-Wen model of hysteresis is often used to describe non-linear hysteretic systems.
FitzHugh-Nagumo model - A hysteretic model of, for example, a neuron.
The hysteretic motion of density waves is therefore not unlike that of dislocations or magnetic domains.
One is the so-called "hysteretic damping model" or "structural damping model".
A simple parametric description of various hysteretic loops may be found in the Lapshin model of hysteresis.
Further experiments, in which they analyzed the history-dependence of the E2F system confirmed that it operates as a hysteretic bistable switch.
Due to the hysteretic effect of water filling and draining the pores, different wetting and drying curves may be distinguished.
The hysteretic Bouc-Wen model has received some criticism regarding its ability to accurately describe the phenomenon of hysteresis in materials.
This drawback is overcome by adding damper, which can be hysteretic materials or a viscous damper.
It is thought that this hysteretic behavior ensures that cells commit to mitosis even if cyclin B1 levels falter.
This model is able to capture, in analytical form, a range of hysteretic cycle shapes matching the behaviour of a wide class of hysteretical systems.
Experimental results prove the ductile, stable and repeatable hysteretic behaviour of structures built with BRBs.
For large resistance junctions the zero-voltage and voltage branches overlap for some range of currents below the critical current, so the device behavior is hysteretic.
That is, the addition of the RC circuit turns the hysteretic bistable multivibrator into an astable multivibrator.
It was introduced by Bouc and extended by Wen, who demonstrated its versatility by producing a variety of hysteretic patterns.