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Musing with GPT-4 on questions about electric current, all the way to string theory
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>> How come electricity signal goes to speed of light? What makes the electrons' wave transmit so | |
fast along a cable? | |
It's a common misconception that electricity or an electrical signal travels at the speed of light. | |
While it's true that electrical signals can travel very fast, they do not reach the speed of light. | |
The speed at which an electrical signal propagates through a conductor like a copper wire or an | |
optical fiber cable is influenced by various factors, such as the material's properties and the | |
surrounding medium. | |
When a voltage is applied to a conductor, the electric field created causes the electrons in the | |
conductor to move. However, the electrons themselves do not travel very fast. Instead, they drift at | |
a slow pace called the "drift velocity," typically much less than 1 mm/s. The reason an electrical | |
signal can travel much faster is that it is not the electrons themselves moving from one end of the | |
wire to the other, but rather the propagation of an electromagnetic wave. | |
This wave is formed by the interaction of the electric and magnetic fields. When a voltage is | |
applied to a conductor, it generates an electric field that in turn creates a magnetic field. These | |
fields interact with one another, forming an electromagnetic wave that propagates through the | |
conductor. This propagation is much faster than the drift velocity of the electrons and can approach | |
a significant fraction of the speed of light, depending on the material and surrounding medium. | |
In a vacuum, the speed of light is about 299,792 km/s (186,282 miles per second). In a typical | |
copper wire, the speed of an electrical signal can be roughly 50-99% of the speed of light, | |
depending on factors like wire composition, insulation, and temperature. In an optical fiber, the | |
signal speed can be even faster, at around 67% of the speed of light, as the signal is transmitted | |
as light rather than an electrical current. | |
So, while the electrical signal does not travel at the speed of light, it can travel very fast due | |
to the propagation of the electromagnetic wave through the conductor, not the movement of the | |
electrons themselves. | |
>> Why is there any drift velocity if the signal is transmitted by an electromagnetic wave? | |
Drift velocity and signal propagation are related but distinct phenomena in the context of electric | |
currents in conductors. Drift velocity is the average velocity at which free electrons in a | |
conductor move under the influence of an electric field. It is a measure of the actual movement of | |
the electrons themselves in response to an applied electric field. | |
When a voltage is applied across a conductor, the electric field created exerts a force on the free | |
electrons in the conductor. These electrons then start to move, colliding with atoms and other | |
electrons in the conductor. Due to these frequent collisions, the electrons move in a random and | |
somewhat slow manner, which results in the relatively low drift velocity. | |
On the other hand, signal propagation refers to the transmission of an electrical signal through a | |
conductor in the form of an electromagnetic wave. The wave is created by the interaction between the | |
electric field and the magnetic field that forms due to the movement of the electrons. This wave | |
travels much faster than the drift velocity of the electrons themselves. | |
So, why is there drift velocity if the signal is transmitted by an electromagnetic wave? The drift | |
velocity represents the actual movement of the electrons, which is necessary to create the | |
electrical current in the conductor. As the electrons move in response to the applied voltage, they | |
create a current that generates the electric and magnetic fields. These fields then interact and | |
propagate as an electromagnetic wave, carrying the electrical signal through the conductor. | |
In summary, drift velocity is related to the movement of electrons, which generates the current and | |
the associated electric and magnetic fields. These fields form an electromagnetic wave, which is | |
responsible for the fast propagation of the electrical signal through the conductor. | |
>> Is all the energy transmitted by an electrical current then coming from the electromagnetic wave? | |
Yes, the energy transmitted by an electrical current is carried by the electromagnetic wave. When an | |
electrical signal is transmitted through a conductor, the energy is conveyed through the interaction | |
between the electric and magnetic fields, which together form an electromagnetic wave. | |
When a voltage is applied across a conductor, the electric field created drives the electrons to | |
move, resulting in an electric current. This current generates a magnetic field, which is | |
perpendicular to the electric field. The two fields are interdependent and influence each other, | |
which creates the electromagnetic wave that propagates through the conductor. | |
The energy associated with this wave is given by the Poynting vector, which describes the flow of | |
electromagnetic energy in a given direction. The Poynting vector is the cross product of the | |
electric field and the magnetic field and is proportional to the product of the electric field | |
strength and the magnetic field strength. | |
The electromagnetic wave carries the energy that is transmitted by the electrical current. This | |
energy can be used to perform work, such as powering electrical devices or generating heat. When the | |
electromagnetic wave reaches the load (e.g., a resistor or an electrical device), the energy is | |
transferred from the wave to the load, which then dissipates the energy as heat or converts it into | |
other forms of energy (such as mechanical or light energy). | |
In summary, the energy transmitted by an electrical current is carried by the electromagnetic wave, | |
which is formed by the interaction between the electric and magnetic fields in the conductor. The | |
energy in the wave is then transferred to the load when the wave reaches it, allowing the load to | |
utilize the energy for various purposes. | |
>> How come then you need to have a closed circuit? What prevents the electromagnetic wave to form | |
if the circuit is open but a voltage is applied to one end? | |
When a voltage is applied to a closed circuit, the electric field generated by the voltage source | |
drives the electrons to move, creating an electric current. This current, in turn, generates a | |
magnetic field, and the interaction between the electric and magnetic fields forms an | |
electromagnetic wave that propagates through the circuit. | |
In an open circuit, however, there is no complete path for the electrons to flow through, which | |
means that no sustained electric current can be established. When a voltage is applied to one end of | |
an open circuit, an electric field is still created, but because the circuit is not closed, the | |
electrons have nowhere to go, and the flow of current is interrupted. | |
While the electric field still exists in the open circuit, the absence of a sustained current means | |
that a magnetic field does not develop as it would in a closed circuit. As a result, there is no | |
interaction between the electric and magnetic fields to form an electromagnetic wave, and thus, no | |
energy can be transmitted through the circuit. | |
In other words, a closed circuit is necessary for the formation of an electromagnetic wave because | |
the closed loop allows for the continuous flow of current, which generates the magnetic field | |
required for the wave to propagate. Without a closed loop, the energy transmission is interrupted | |
due to the lack of a sustained current and the associated magnetic field. | |
>> But since the drift velocity is so low how come the the current appears immediately as you close | |
the circuit | |
Although the drift velocity of electrons is very low, the current appears to flow almost | |
instantaneously when you close a circuit because of the way electric fields propagate through the | |
conductor. | |
When you close the circuit, the voltage applied to the conductor creates an electric field that | |
extends through the entire circuit. This electric field exerts a force on the free electrons in the | |
conductor, causing them to move. Although the actual movement of the electrons (drift velocity) is | |
slow, the electric field itself propagates through the conductor at a much faster speed, close to | |
the speed of light for the material. | |
As the electric field propagates, it influences the motion of electrons throughout the entire length | |
of the conductor. This means that electrons near the positive terminal of the voltage source start | |
moving almost at the same time as electrons near the negative terminal. The overall effect is that | |
when you close the circuit, the current appears to flow immediately, even though the electrons | |
themselves are moving at a relatively slow drift velocity. | |
In essence, the near-instantaneous appearance of the current is due to the fast propagation of the | |
electric field, which affects the motion of electrons throughout the conductor simultaneously. This | |
rapid propagation allows the current to be established quickly, even though the actual movement of | |
the electrons is much slower. | |
>> Okay. Now how come we can have an eletric field (since light is an electromagnetic wave as well) | |
in vacuum? | |
Electromagnetic waves, such as light, can indeed propagate through a vacuum. In contrast to electric | |
currents in a conductor, which rely on the flow of electrons, electromagnetic waves can travel | |
through empty space because they consist of oscillating electric and magnetic fields that are | |
self-sustaining and do not require a material medium to propagate. | |
An electromagnetic wave is formed by the interaction of an electric field and a magnetic field, | |
which are both perpendicular to each other and to the direction of wave propagation. These fields | |
continuously generate each other in a self-sustaining manner, allowing the wave to travel through | |
space. | |
The propagation of an electromagnetic wave through a vacuum can be understood using Maxwell's | |
equations, a set of four fundamental equations that describe the behavior of electric and magnetic | |
fields. Two key aspects of these equations explain why electromagnetic waves can propagate through a | |
vacuum: | |
- A changing electric field generates a magnetic field. | |
- A changing magnetic field generates an electric field. | |
As the electric field oscillates, it produces a changing magnetic field, which in turn generates a | |
changing electric field. This process repeats continuously as the electromagnetic wave propagates | |
through the vacuum. Since the electric and magnetic fields can create each other without the need | |
for a material medium, electromagnetic waves can travel through empty space. | |
This property of electromagnetic waves allows them to propagate across vast distances in space, such | |
as light from distant stars and galaxies reaching Earth or radio signals transmitted between | |
satellites and ground stations. | |
>> But what supports the eletric and magnetic fields if there is not matter. Is that a property of | |
space itself? | |
Yes, the ability of electromagnetic waves to propagate through a vacuum can be thought of as a | |
property of space itself. The electric and magnetic fields in an electromagnetic wave don't require | |
matter to exist and interact. They are self-sustaining and can propagate through empty space due to | |
the fundamental principles of electromagnetism described by Maxwell's equations. | |
In classical physics, empty space, or vacuum, is considered a stage or a backdrop where physical | |
processes and interactions occur. Although a vacuum is devoid of matter, it still allows for the | |
existence and propagation of electric and magnetic fields, which are intrinsic to the fabric of | |
spacetime itself. | |
The concept of fields is crucial in physics. Fields are mathematical constructs that represent the | |
distribution of certain quantities, such as electric or magnetic force, throughout space. They help | |
us understand how particles or objects interact with each other over distances without direct | |
contact. | |
In the case of electric and magnetic fields, they permeate and influence the vacuum of space, | |
enabling the propagation of electromagnetic waves. This is different from mechanical waves, like | |
sound waves, which require a material medium (air, water, or solid) to transmit energy through the | |
vibrations of particles in the medium. | |
In summary, the ability of electric and magnetic fields to exist and interact in a vacuum can be | |
considered a fundamental property of space itself. These fields do not require the presence of | |
matter to support their existence, and they allow electromagnetic waves to propagate through empty | |
space according to the principles of electromagnetism. | |
>> Are there generalization of general relativity theory to electric and magnetic field, that is, | |
framing them as a distortion of space time vs just a "force" ? | |
Yes, there have been attempts to generalize the concepts of general relativity to incorporate | |
electric and magnetic fields, often referred to as "electromagnetic gravity" theories. The aim of | |
these theories is to unify the description of electromagnetic fields and gravity within a single | |
geometric framework. | |
One such approach is the Kaluza-Klein theory, originally proposed by Theodor Kaluza in 1921 and | |
later extended by Oskar Klein. This theory suggests that the fundamental forces, including gravity | |
and electromagnetism, can be described within a higher-dimensional spacetime. In the case of | |
Kaluza-Klein theory, a 5-dimensional spacetime is considered, with one of the dimensions being | |
compactified or "curled up" at a very small scale. When this extra dimension is included, the | |
higher-dimensional version of Einstein's field equations can describe both gravity (in the form of | |
spacetime curvature) and electromagnetism. | |
Another approach involves the concept of "gauge fields" in particle physics. In this framework, the | |
electric and magnetic fields can be described as gauge fields associated with the electromagnetic | |
force, which is mediated by photons. These gauge fields are responsible for the interactions between | |
charged particles, much like the gravitational field is responsible for the interactions between | |
masses. In some theoretical models, the geometric description of gravity is extended to include | |
these gauge fields, potentially leading to a unified description of gravity and electromagnetism. | |
However, it is essential to note that these are theoretical attempts to find a unified description, | |
and none of them have been experimentally confirmed or widely accepted as a complete description of | |
the relationship between gravity and electromagnetism. The search for a consistent and | |
experimentally verifiable theory that unifies all fundamental forces, including gravity, | |
electromagnetism, the strong nuclear force, and the weak nuclear force, is still an active area of | |
research in theoretical physics. | |
>> Are these two theories kind of similar to string theory? Basically the premises being to add new | |
dimensions to extend Einstein's field equations to unify all forces we observe in nature? | |
Yes, the Kaluza-Klein theory and string theory share some similarities, as both approaches involve | |
adding extra dimensions to extend Einstein's field equations and attempt to unify the fundamental | |
forces of nature. While the Kaluza-Klein theory specifically focuses on unifying gravity and | |
electromagnetism in a 5-dimensional spacetime, string theory is a broader framework that attempts to | |
describe all fundamental forces and particles in terms of one-dimensional, vibrating strings. | |
String theory posits that all particles and forces, including gravity, electromagnetism, the strong | |
nuclear force, and the weak nuclear force, are manifestations of different vibrational modes of | |
these fundamental strings. To accommodate these vibrations and the interactions between strings, | |
string theory requires the existence of additional dimensions beyond the familiar four dimensions of | |
spacetime (three spatial dimensions and one time dimension). | |
Depending on the specific version of string theory, the number of dimensions can range from 10 to | |
26. The extra dimensions are often assumed to be compactified or "curled up" at extremely small | |
scales, making them undetectable in everyday experiences and experiments. The idea of compactified | |
dimensions in string theory is reminiscent of the extra dimension in the Kaluza-Klein theory. | |
The main difference between the Kaluza-Klein theory and string theory lies in the scope and the | |
underlying principles. The Kaluza-Klein theory is focused on unifying gravity and electromagnetism | |
in a higher-dimensional spacetime, whereas string theory is a more comprehensive framework that | |
attempts to describe all particles and forces in terms of vibrating strings in higher-dimensional | |
spacetimes. | |
Despite these similarities, it is important to note that string theory is still a theoretical | |
framework with no direct experimental confirmation. While it has produced some intriguing and | |
elegant mathematical results, the search for a consistent and experimentally verifiable theory that | |
unifies all fundamental forces remains an ongoing pursuit in theoretical physics. | |
>> Why does string theory require the introduction of the concept of strings? With a sufficient | |
number of dimensions can't we emulate any force field with Einstein's field equations? | |
The introduction of strings in string theory is not merely a consequence of adding extra dimensions | |
to spacetime. Instead, the concept of strings arises from the attempt to solve some inherent issues | |
in the existing theoretical frameworks, particularly the incompatibilities between general | |
relativity and quantum mechanics. | |
General relativity, which is based on Einstein's field equations, is a classical theory that | |
describes gravity as the curvature of spacetime caused by the presence of mass-energy. It has been | |
extremely successful in explaining gravitational phenomena at macroscopic scales. However, when | |
applied to extremely small scales or high-energy situations, general relativity is not compatible | |
with quantum mechanics, which governs the behavior of particles and forces at the subatomic level. | |
One of the primary issues in combining general relativity and quantum mechanics is the problem of | |
infinities that arise when trying to quantize the gravitational force. These infinities make it | |
difficult to develop a consistent quantum theory of gravity. String theory is an attempt to address | |
these problems by replacing point-like particles with one-dimensional, vibrating strings. | |
In string theory, the fundamental particles and forces are described as different vibrational modes | |
of these strings. The strings have a finite length, which helps to avoid the infinities that plague | |
the quantization of gravity in a point-particle framework. The introduction of extra dimensions in | |
string theory is necessary to accommodate the various vibrational modes and interactions between | |
strings. | |
While adding extra dimensions to spacetime can provide a unified description of gravity and | |
electromagnetism, as demonstrated by the Kaluza-Klein theory, it does not automatically resolve the | |
issues related to quantum mechanics and general relativity. The concept of strings in string theory | |
is a key element in addressing these issues and developing a consistent quantum theory of gravity | |
that incorporates all fundamental forces. | |
In summary, the introduction of strings in string theory is not just a byproduct of adding extra | |
dimensions, but a fundamental aspect of the theory that aims to resolve the incompatibilities | |
between general relativity and quantum mechanics. |
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