Electromagnetism Lecture#8 Instructor: Engr. Muhammad Mateen Yaqoob.

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Electromagnetism Lecture#8 Instructor: Engr. Muhammad Mateen Yaqoob

Transcript of Electromagnetism Lecture#8 Instructor: Engr. Muhammad Mateen Yaqoob.

Page 1: Electromagnetism Lecture#8 Instructor: Engr. Muhammad Mateen Yaqoob.

ElectromagnetismLecture#8

Instructor:

Engr. Muhammad Mateen Yaqoob

Page 2: Electromagnetism Lecture#8 Instructor: Engr. Muhammad Mateen Yaqoob.

Magnetic Fields In 1269 a Frenchman named Pierre de Maricourt found that directions of a needle near a spherical natural magnet formed lines that encircled sphere and passed through two points diametrically opposite each other, which he called poles of magnet.

Subsequent experiments showed that every magnet, regardless of its shape, has two poles, called north (N) and south (S) poles, that exert forces on other magnetic poles similar to way that electric charges exert forces on one another.

Poles received their names because of way a magnet, such as that in a compass, behaves in presence of Earth’s magnetic field.

MATEEN YAQOOB DEPARTMENT OF COMPUTER SCIENCE

Page 3: Electromagnetism Lecture#8 Instructor: Engr. Muhammad Mateen Yaqoob.

Magnetic Fields Although force between two magnetic poles is otherwise similar to force between two electric charges, electric charges can be isolated (witness electron and proton) whereas a single magnetic pole has never been isolated. That is, magnetic poles are always found in pairs.

MATEEN YAQOOB DEPARTMENT OF COMPUTER SCIENCE

Page 4: Electromagnetism Lecture#8 Instructor: Engr. Muhammad Mateen Yaqoob.

Magnetic Fields and Forces In our study of electricity, we described interactions between charged objects in terms of electric fields.

In addition to containing an electric field, region of space surrounding any moving electric charge also contains a magnetic field.

A magnetic field also surrounds a magnetic substance making up a permanent magnet.

Symbol B has been used to represent a magnetic field. Direction of magnetic field B at any location is direction in which a compass needle points at that location.

MATEEN YAQOOB DEPARTMENT OF COMPUTER SCIENCE

Page 5: Electromagnetism Lecture#8 Instructor: Engr. Muhammad Mateen Yaqoob.

Magnetic Fields and Forces We can represent magnetic field by means of drawings with magnetic field lines.

MATEEN YAQOOB DEPARTMENT OF COMPUTER SCIENCE

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Defining a magnetic field We can define a magnetic field B at some point in space in terms of the magnetic force FB that field exerts on a charged particle moving with a velocity v, which we call test object.

Experiments on various charged particles moving in a magnetic field give following results:

1. Magnitude FB of magnetic force exerted on particle is proportional to charge q and to speed v of particle.

2. Magnitude and direction of FB depend on velocity of particle and on magnitude and direction of magnetic field B.

3. When a charged particle moves parallel to magnetic field vector, magnetic force acting on particle is zero.

MATEEN YAQOOB DEPARTMENT OF COMPUTER SCIENCE

Page 7: Electromagnetism Lecture#8 Instructor: Engr. Muhammad Mateen Yaqoob.

Defining a magnetic field

4. When particle’s velocity vector makes any angle θ (non-zero) with magnetic field, magnetic force acts in a direction perpendicular to both v and B; that is, FB is perpendicular to plane formed by v and B.

5. Magnetic force exerted on a positive charge is in direction opposite direction of magnetic force exerted on a negative charge moving in same direction.

6. Magnitude of magnetic force exerted on moving particle is proportional to sinθ, where θ is angle particle’s velocity vector makes with direction of B.

MATEEN YAQOOB DEPARTMENT OF COMPUTER SCIENCE

Page 8: Electromagnetism Lecture#8 Instructor: Engr. Muhammad Mateen Yaqoob.

Defining a magnetic field We can summarize these observations by writing magnetic force in form:

SI unit of magnetic field is newton per coulomb-meter per second, which is called Tesla (T)

A non-SI magnetic-field unit in common use, called gauss (G), is related to tesla through conversion 1T= 104 G

MATEEN YAQOOB DEPARTMENT OF COMPUTER SCIENCE

Page 9: Electromagnetism Lecture#8 Instructor: Engr. Muhammad Mateen Yaqoob.

MATEEN YAQOOB DEPARTMENT OF COMPUTER SCIENCE

Ampere’s Law We have seen that moving charges or currents are the source of magnetism. This can be readily demonstrated by placing compass needles near a wire. As shown in Figure, all compass needles point in the same direction in the absence of current. However, when I is non zero, the needles will be deflected along the tangential direction of the circular path.

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MATEEN YAQOOB DEPARTMENT OF COMPUTER SCIENCE

Page 11: Electromagnetism Lecture#8 Instructor: Engr. Muhammad Mateen Yaqoob.

MATEEN YAQOOB DEPARTMENT OF COMPUTER SCIENCE

Page 12: Electromagnetism Lecture#8 Instructor: Engr. Muhammad Mateen Yaqoob.

MATEEN YAQOOB DEPARTMENT OF COMPUTER SCIENCE

Page 13: Electromagnetism Lecture#8 Instructor: Engr. Muhammad Mateen Yaqoob.

MATEEN YAQOOB DEPARTMENT OF COMPUTER SCIENCE

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MATEEN YAQOOB DEPARTMENT OF COMPUTER SCIENCE

Magnetic flux (Φ) The group of force lines going from north pole to south pole of a magnet is called magnetic flux

Number of lines of force in a magnetic field determines the value of flux

Unit of magnetic flux is Weber (Wb)

One weber is 108 lines

It is a huge unit; so in most of applications micro-weber (µWb) is used

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MATEEN YAQOOB DEPARTMENT OF COMPUTER SCIENCE

Magnetic flux density (B) It is the amount of flux per unit area perpendicular to the magnetic field

Its symbol is B and its unit is Tesla (T)

One tesla equals one weber per square meter (Wb/m2)

B = Φ / A

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MATEEN YAQOOB DEPARTMENT OF COMPUTER SCIENCE

Faraday’s Law The electric fields and magnetic fields considered up to now have been produced by stationary charges and moving charges respectively.

Imposing an electric field on a conductor gives rise to a current which in turn generates a magnetic field.

In 1831, Michael Faraday discovered that, by varying magnetic field with time, an electric field could be generated. The phenomenon is known as electromagnetic induction.

Faraday’s experiment demonstrates that an electric current is induced in the loop by changing the magnetic field.

The coil behaves as if it were connected to a source.

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MATEEN YAQOOB DEPARTMENT OF COMPUTER SCIENCE

Consider a uniform magnetic field passing through a surface S

The magnetic flux through the surface is given by

Faraday’s law of induction may be stated as:

The induced emf ε in a coil is proportional to the negative of the rate of change of magnetic flux

For a coil that consists of N loops