Parameter Variation Machines

Description: Understanding the concept of hysteresis is crucial. Generally, this phenomenon leads to losses observed in the dielectric of a capacitor or the lamination of a transformer, which can manifest as heat (emission of infrared photons). Alternatively, it can extract work from a circuit without corresponding heat loss (a new type of loss not commonly described in textbooks) and, conversely, impart work to the circuit from the cooling of the environment surrounding the circuit element (absorption of infrared photons). In theoretical investigations of electric induction, the propagating velocity of the transverse electromagnetic (TEM) component of induction is the only propagation constant considered. However, in reality, the independent magnetic field of induction and the independent dielectric field of induction begin at the conductor and propagate through space at a specific velocity. At any point in space, the field of induction of magnetism or dielectricity at any moment corresponds not to the condition of induction at the conductor at that moment but to a moment earlier, determined by the time it takes for the induction to propagate from the conductor to the point in space under consideration. Consequently, the field of induction lags in time more significantly the greater the distance from the conductor. This phase lag results in the cycle of energy return of the field of induction falling behind its point of phase opposition with the cycle of energy storage. This phase lag introduces an energy component, effectively creating a magnetic resistance or dielectric conductance to the reactance or susceptance of the magnetic and dielectric fields, respectively. The phase angle of this lag in the energy return cycle is referred to as the hysteresis angle of the inductive medium, which is well-known for ferrous materials. However, the application of this concept to the inductive medium known as the aether has received little attention, aside from Steinmetz's work. The purpose of this study is to adapt Steinmetz's inductive propagation to the examination of the hysteresis of the aether and to determine the propagation velocity from this analysis. Referring back to Heaviside's work, there exists the H field or "intrinsic magnetization" and the B field or "induced magnetization." The H field is considered the applied field, while the B field is the resultant field, leading to the older term "magnetic induction" for B. Heaviside emphasizes that the B field and H field do not necessarily follow one another and typically exhibit a time lag between them. This phenomenon is generally termed hysteresis, which can consume (usually occurs) or produce (rarely occurs) electrical energy. Mr. Dollard has highlighted this on the forum and in his published works, but it was only recently that a comprehensive understanding of these concepts emerged. It appears that Heaviside inadvertently uncovered the foundation for the actions in which synchronous parametric variation may operate, at least concerning the magnetic circuit. Although he was addressing a different subject, it is intriguing to reflect on this in the context of parametric variation of inductance. A deep understanding of the concept of hysteresis (the lagging of an effect behind its cause) is essential, as it leads to losses in the dielectric of capacitors or transformer laminations, observable as heat (infrared photon emission). Alternatively, it can extract work from a circuit without associated heat loss (a new form of loss not typically described in textbooks) and can impart work to the circuit through the cooling of the surrounding environment (infrared photon absorption).

The phenomenon of hysteresis plays a significant role in the behavior of electronic components, particularly in inductive and capacitive devices. In capacitors, hysteresis losses arise from the dielectric material's inability to instantly respond to an alternating electric field, resulting in energy dissipation as heat. This is particularly relevant in applications where capacitors are subjected to high-frequency signals, as the dielectric material's characteristics can lead to increased losses, impacting the overall efficiency of the circuit.

In transformers, hysteresis losses are primarily attributed to the magnetic core material. The alternating magnetic field induces magnetization in the core, but due to hysteresis, the magnetization does not perfectly follow the applied magnetic field. This lag results in energy losses as heat, which can affect the performance and thermal management of the transformer. The choice of core material, its shape, and lamination can significantly influence hysteresis losses, making material selection critical for optimizing transformer efficiency.

Understanding the implications of hysteresis extends beyond just losses; it also provides insights into the design and operation of circuits. For instance, the phase lag between the H and B fields can be utilized in applications such as inductive heating, where controlled hysteresis can generate heat efficiently. Additionally, in advanced applications such as synchronous parametric variation circuits, recognizing the hysteresis effects can lead to innovative designs that exploit these characteristics for improved performance.

In summary, hysteresis is a complex phenomenon with far-reaching implications in electronics. It is essential for engineers and designers to consider hysteresis effects in their designs to mitigate losses and enhance the performance of electronic devices. Understanding the underlying principles of hysteresis will facilitate the development of more efficient and effective electronic systems.Understanding of the concept of "Hysteresis" is very important. When generally considered, this phenomena gives rise to losses seen in the dielectric of a capacitor or lamination of a transformer, these can be seen in the form of heat(emission of infrared photons). Alternatively it can remove work from a circuit without associated heat loss (a new form of loss not described in any common textbook),

and oppositely impart work to the circuit from cooling of the environment surrounding the cicuit element (absorption of infrared photons). In the theoretical investigation of electric induction the propagating velocity of the transverse electro-magnetic (T.

E. M. ) component of induction is the only propagation constant considered. The propagation throughout space of the independent magnetic field of induction and the independent dielectric field of induction is not considered. In reality, however, these fields of induction start at the conductor and propagate from there throughout space at a definite velocity; that is, at any point in space the field of induction of magnetism or dielectricity at any moment in time corresponds not to the condition of induction at the conductor at that moment but that at a moment earlier by the time of propagation from the conductor to the point in space under consideration.

Hence the given field of induction lags in time the more, the greater the distance from the conductor. This lag in phase with respect to distance results in the cycle of energy return of the field of induction falling behind its point of phase opposition with the cycle of energy storage.

This lag in phase gives rise to an energy component, that is an effective magnetic resistance or an effective dielectric conductance to the reactance or susceptance of the magnetic & dielectric fields respectively. The phase angle of this lag in the cycle of energy return has been called the angle of hysteresis of the inductive medium and has become well known for ferrous materials.

However, the application of this concept to the inductive medium known as the aether has received no attention except by Steinmetz. The purpose of this paper is the adaptation of Steinmetz` inductive propagation to the study of the hysteresis of the aether and a determination of the propagation velocity therefrom.

Going back to Heaviside`s work, we have the H field or "intrinsic magnetization" and the B field or the "induced magnetization". H was considered the applied field and B the resultant field and hence the older term "magnetic induction" for B.

Heaviside points out that the B field and H field do NOT have to follow one another and usually do have a time lag between one another. This phenomena is generally called hysteresis, this HYSTERESIS is something that can consume (usually happens) or produce (rarely happens) electrical energy.

Mr. Dollard has pointed this out here on the forum and in his published works, but it wasn`t until recently that it all came together in my head. It would seem Heaviside inadvertently discovered the basis for the actions in which synchronous parametric variation may work, at least for the magnetic circuit.

While he is talking about another subject its funny to read that and not think of parametric variation of an inductance. I feel a deep understanding of the concept of "Hysteresis" (the lagging of an effect behind its cause) is very important.

When generally considered, this phenomena gives rise to losses seen in the dielectric of a capacitor or lamination of a transformer, these can be seen in the form of heat (emission of infrared photons). Alternatively it can remove work from a circuit without associated heat loss (a new form of loss not described in any common textbook), and oppositely impart work to the circuit from cooling of the environment surrounding the circuit element (absorption of infrared photons).

In the theoretical investigation of