firdiana sanjaya 4201414050 ana alina 4201414095

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Firdiana Sanjaya 4201414050 Ana Alina 4201414095

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Page 1: Firdiana Sanjaya 4201414050 Ana Alina 4201414095

Firdiana Sanjaya 4201414050

Ana Alina 4201414095

Page 2: Firdiana Sanjaya 4201414050 Ana Alina 4201414095

MagnetismEvery magnet of whatever shape has two poles,designated the north and south poles

The like poles of two magnets repel each other and the unlike poles attrack each other.

With a typical bar magnet, for example, the field goes from the north pole to the south pole outside the magnet, and back from south to north inside the magnet.

The relationship between magnetism and electricity shown that a changing magnetic field creates an electric field and a changing electric field creates a magneticfield.

Page 3: Firdiana Sanjaya 4201414050 Ana Alina 4201414095
Page 4: Firdiana Sanjaya 4201414050 Ana Alina 4201414095

The magnetic field produced by currents in wires The magnitude of the field at a distance r from a wire carrying a

current I is given by:

The field at the center of a circular loop of radius r carrying a current I is given by:

For N loops put together to form a flat coil, the field is just multiplied by N:

The field along the axis of the solenoid has a magnitude of:

Page 5: Firdiana Sanjaya 4201414050 Ana Alina 4201414095

Right-hand rule

the vector v is in the direction of your thumb and B in the direction of your fingers. The force FB on a positive charge is in the direction of your palm, as if you are pushing the particle with your hand.

Page 6: Firdiana Sanjaya 4201414050 Ana Alina 4201414095

The force on a charged particle in a magnetic fieldExperiments on various charged particles moving in a magnetic field give the following results: The magnitude FB of the magnetic force

exerted on the particle is proportional to the charge q and to the speed v of the particle.

The magnitude and direction of FB depend on the velocity of the particle and on the magnitude and direction of the magnetic field B.

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

Page 7: Firdiana Sanjaya 4201414050 Ana Alina 4201414095

When the particle’s velocity vector makes any angle ≠ 0 with the magnetic field, the magnetic force acts in a direction perpendicular to both v and B; that is, FB is perpendicular to the plane formed by v and B

The magnetic force exerted on a positive charge is in the direction opposite the direction of the magnetic force exerted on a negative charge moving in the same direction

The magnitude of the magnetic force exerted on the moving particle is proportional to sin , where is the angle the particle’s velocity vector makes with the direction of B.

Page 8: Firdiana Sanjaya 4201414050 Ana Alina 4201414095

Magnetic Force Acting on a Current-Carrying Conductor

B directed out of the page

B directed into the page

DIRECTION OF B

Page 9: Firdiana Sanjaya 4201414050 Ana Alina 4201414095

Magnetic Force Acting on a Current-Carrying Conductor

Page 10: Firdiana Sanjaya 4201414050 Ana Alina 4201414095

Torque on a Current Loop in a Uniform Magnetic Field

For the magnetic field is parallel to the plane of the loop

Page 11: Firdiana Sanjaya 4201414050 Ana Alina 4201414095

For the uniform magnetic field makes an angle 90° with a line perpendicular to the plane of the loop

Torque on a Current Loop in a Uniform Magnetic Field

Page 12: Firdiana Sanjaya 4201414050 Ana Alina 4201414095

Although we obtained the torque for a particular orientation of B with respect to the loop, the equation x B is valid for any orientation. Furthermore, although we derived the torque expression for a rectangular loop, the result is valid for a loop of any shape.

If a coil consists of N turns of wire, each carrying the same current and enclosing the same area, the total magnetic dipole moment of the coil is N times the magnetic dipole moment for one turn.

The potential energy of a system of a magnetic dipole in a magnetic field depends on the orientation of the dipole in the magnetic field and is given by

Torque on a Current Loop in a Uniform Magnetic Field

Page 13: Firdiana Sanjaya 4201414050 Ana Alina 4201414095

Motion of a Charged Particle in a Uniform Magnetic Field

The particle moves in a circle because the magnetic force FB is perpendicular to v and B and has a constant magnitude qvB. As Figure illustrates, the rotation is counterclockwise for a positive charge. If q were negative, the rotation would be clockwise.

Page 14: Firdiana Sanjaya 4201414050 Ana Alina 4201414095

The Cyclotron A cyclotron is a device that can accelerate charged particles to very

high speeds. The energetic particles produced are used to bombard atomic nuclei and thereby produce nuclear reactions of interest to researchers.

A cyclotron consists of an ion source at P, two dees D1 and D2 across which an alternating potential difference is applied, and a uniform magnetic field.(The south pole of the magnet is not shown.) The red dashed curved lines represent the path of the particles.

Page 15: Firdiana Sanjaya 4201414050 Ana Alina 4201414095

The Hall Effect When a current-carrying conductor is placed in a

magnetic field, a potential difference is generated in a direction perpendicular to both the current and the magnetic field.This phenomenon is known as the Hall effect.

Page 16: Firdiana Sanjaya 4201414050 Ana Alina 4201414095

The Hall Effect

Page 17: Firdiana Sanjaya 4201414050 Ana Alina 4201414095

THANKS

Page 18: Firdiana Sanjaya 4201414050 Ana Alina 4201414095

QUESTION

Andika

How to get this formula : Lakha

What is the direction of magnetic field? Is that from north to south? Hanif

How can magnetic field create electric field?