Heisenberg Uncertainty Principle

Heisenberg a German scientist stated the principle of uncertainty which is consequence of dual nature of the matter and waves.
the Heisenberg uncertainty principle state that it is possible to find on the position and momentum of an electron at the same moment.

Mathematically representations of this is follows

Delta of X into delta of the less than equal to h/4nm

Delta X is the uncertainty of a positions of electron

Delta b x is uncertainty of the momentum that is called velocity.

h is equal to planck constant.

M equal to masses.

you know the positions of electrons with the high quality then its velocity will be will be uncertain.

Similarly if the velocity of the electron is notch preciously then its position will be uncertain.

The exact picture of the both Momentum and position will never be clear.

This is the main concept of the principle of uncertainty.

Important of uncertainty principle

The uncertainty principle is rules out
The concept of defined path and trajectories of electrons.

The path of object is determined by its length at various instant of time.

if the exact location of a particle is known along with its velocity at that instant and the forces acting on it is the similar particle to be determined even after sometime.

it can be concluded that the position and velocity of a particle and the forces acting upon it is a n trajectory.

as we cannot famine translate determine the position and velocity of subatomic particle size is electrons it is impossible to talk about the trajectory. the project of Heisenberg Uncertainty Principle CCB significant only for the motion of microscope object.
it is negligible in case of this microscopic object for example to apply the concept of uncertainty to an object of masses of one milligram.

no more about the Heisenberg Uncertainty Principle formula we have to find out different phases.

Einstein field equation

Einstein field equations also known as Einstein equation they are all the set of that 10 equation extracted from the Albert Einstein general theory of relativity.

the Einstein field equations describe the basic introductions of gravitation equations first published in 1915 by Albert Einstein is a tensor equation.

the Einstein field equations are determined by the space time geometry of the space present age of the energy images of Linear Momentum this is the same equations where the electromagnetic field or identified by the current and charges.

dynasty and field equations was first formulated in the four dimensional theory that some tourist explore it i
as n dimensionals.

How was the general theory of relativity are also referred as Einstein field equations.
in this equation sahuli return out they are the systems of 10 nominal coupled hyperbolic elliptic differential equation.
This equation defined in the Einstein field theory..

Faraday's law

When we study the topics of electromagnetism we come across one of the important lodge that is called Faraday's laws which basically describes the key point leading to the practical generation of electricity or electromagnetic induction.

the law was proposed in the year 1831 by the experimental physicist and chemist named Michael Faraday.

so you can see why the name of the lord is come from that being said the blood is low or the laws of electromagnetic induction is always equal in the result of the observation of the experimental at that point of time .

He performed three main experiment to discover the phenomenon of electromagnetic induction.

Relationship between the induced EMF or flux.

in the first experiment he proved that when the strength of the magnetic field is embedded in a leader induced current is produced an ammeter is connected to the law of the wire animated deflected when the magnetic was move toward the wire.

In the second experiment he proved that passing a current through an iron rod would make it electromagnetic.
he observed that when there is a relative motion exist between the magnet and the coil The induced electromotive force is created.

when the magnet was rotated about its Axis no electromagnetic force was observed cut off when the magnet was rotated about its own axis then the induced electromotive force  was produced.
Does there was no deflection in the emitted when the magnet was held stationary.

while conducting the third experiment he recorded that the Galvanometer did not so any deflection and no induced current was produced in the coil when the coil was moved in a station a magnetic field. bimetal deflected in the opposite direction when the magnet was moved away from the loop.

The positions of magnet

Magnet at rest

No deflection in the galvanometer

Magnet moves towards the coil

Deflection in the Galvanometer in one direction

Magnet is held stationary at the same position

No deflection galvanometer

Magnet moves away from the coil

Deflection in the Galvanometer but the opposite direction.

Magnet held stationary at the same position

No deflection in galvanometer.

conclusion after conducting all experiment Heritage finally concluded that if the relative motion suggested between a conductor in a magnetic field attracts linkage with a coil change this and these changes in the class produced voltage across the coil.

Ramesh lodge basically states of when the magnetic flask for the magnetic field changes with the time the electromotive force is produced additional Michael Faraday also permitted to launch on the basis of above experiment.

Faraday's first law

what is first law of electromagnetic induction system that the whenever a conductor is placed in the varying magnetic field the electromagnetic field produced induced electromotive force.

if the conductor circuit is closed a current is also induced which are called induced current

A way of charging magnetic field

By rotating the coil related to the magnet.

By moving the coil in 2 or out of the magnetic field.

By changing the area of a coin placed in the magnetic field.

Lagrangian point

lund Ranjan. Is defined as the point that is near to large body is Inorbit such that the smaller object maintains its position relative to the large orbiting bodies.

Lagrangian point is also known as l. All languages point Or libration point.

Fourier's Law

tourist lodge state that the negative gradient of temperature and the time rate of heat transfer or proportional at to the area at right angles of that gradient through who is the heat flows.

Fourier's law is another name of the law of heat conduction.

Differential form of Fourier's law

Fourier's law in differential form as follows equal to minus K Delta T Q equal to local heat flux density in w b square is equal to conductivity of the material in w per metre square per Kelvin Delta temperature gradient in kelvin parameter in the one dimensional problem

Curie-wriss law

The curie Weiss law is one of important law in the electromagnetism that says that the magnetic susceptibility is above the Curie temperature. At of the ferromagnetism in the paramagnetic.

the magnetic moment is a quantity of the magnet that determines its work in an external magnetic field.

For example a bar magnet electric current loop molecules and and electrons all have a magnetic moment.

the magnetic polarizations Aaye Nagar positions of the magnetic material expresses the density of induced or permanent magnetic moment in the vector field.

the magnetic moments can develop from the microscopic electric current that is generated by the spin of electrons or motions of electrons in an atom or the speed of the nuclei.

sequel to material specific Uri tikuli Absolute Temperature NTC kallikudi temperature the net magnetization dependent on the respond of the external magnetic field material how but they maybe even present in the absence of the external magnetic field for example in a cold drawn as a spontaneous magnetization.

while other materials have the similar property of the magnetic and the Nicholas II the ferrimagnetism the temperature at which a ferromagnetic material is called Curie temperature.

The laws of conservation of linear momentum

the linear momentum of the particle at an instance is defined as the product is of its message and velocity of the particle and tenses table representation by the symbol speak and it is a vector quantity.

P equal to Mv
Where p=mv

The momentum of a system of a particle is the vector sum of the individual momentum of all the particles.

Law of conservation of linear momentum

if the net external forces acting on a systems of body is zero then the momentum of the systems remain constant.

This is the basic laws of conservation of linear momentum.

we have to remember that this moment of resistance is observed and not that the individual particle government of individual bodies in the systems might increase of the decrease according to the situation but the moment of the systems you'll always be conserved as long as there is no external forces acting on it.

explanation the law of conservation of momentum can be explained from the second law of motion Newton's second law of the motion says that the rate of changes of linear momentum of a body is equal to the net external forces applied .

if the external forces acting on a body is zero then the rate of changes of the momentum is also zero which means that a force is no changes in momentum.

the bodies of the masses M and M are moving opposite directions with a velocity V if the collided of the moment together after the collision so I have to find the security of the systems.

she is there is no external forces acting on the systems of the body is Momentum will be conserved initial Momentum equal to final momentum.

From this occasion we can easily find the final momentum.

one of the application of the conservation of momentum is it gets pushed toward and motorized concept Momentum.

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