MAGNETISM
CONCEPT
It is part of physics that studies the properties of magnets. These properties are manifested by some minerals such as iron, cobalt, nickel, steel, etc. Best known for their magnetic properties is the mineral magnetite (Fe3O4).
Magnets are objects that enjoy two important properties:
1. Attract iron. In this sense, some substances such as steel or metal alloys in weak become permanent magnets when placed near a natural magnet for a certain time. Then they say the substances are magnetized.
2.- Oriented in a particular
direction in space. For example when iron filings are sprinkled near a
bar-shaped magnet, these iron filings group forming specific lines.
3. The ends of the magnet are
called magnetic poles or poles of the magnet, which is where external magnetic
effects of the magnet are concentrated, there greater accumulation of iron
filings appear.
The concentration of these poles
in the magnet are at a distance from the ends of the magnet equivalent to 1/12
of the length of the magnet.
The pole that is oriented to the
geographic north is called north magnetic pole (N), the other is called south
magnetic pole (S), and the intermediate part is called neutral zone.
If you have a magnetized iron rod
and it is suspended by a thread in its central part, it tends to align with the
north-south direction; from this we can also understand the ordinary compass
whose needle is just a piece of magnetized iron.
4. The same poles repel each other
and opposite poles attract each other.
5. An electric current creates a
magnetic field in the surrounding space, and this action affects near objects
without touching them.
The following graph shows a case
where a electric current flows through a conductor wire, which perpendicularly
intersects a plane, in this case a paper, which has been sprinkled with iron
filings that are oriented along concentric circular paths . These geometric
paths are called "lines of magnetic induction," which graphically
represent the magnetic field that surrounds the conductor wire.
Loss of magnetic properties
A magnet can lose their magnetic
properties due to two reasons:
1. When it is heated up to a
certain temperature, which is known with the name Curie temperature.
Iron.......750oC
Ferrite...218oC
Nickel...350oC
2. When it's hit, since it can
produce a molecular disorder.
Inseparability of the poles
If a magnet is cut into two parts,
each of the portions obtained constitute a new magnet, and that means with its
own north pole and south pole. And this incident may continue until the
molecular level, so that a molecule with magnetic polarity comes to be called
molecular magnet.
In the atomic theories of matter
and quantum mechanics, it's said that microscopic currents exist and are
associated with the movement of electrons around the nucleus of the atom and
the electron spin, which means a type of rotation of the electron on its own
axis.
LAWS OF MAGNETISM
Qualitative law
External magnetic poles of the
same name repel and the ones of different name attract each other.
Quantitative law
The law states that the force of
attraction or repulsion between two magnetic poles is directly proportional to
the product of the intensities of the magnetic poles and inversely proportional
to the square of the distance between them.
Where
F: Force of magnetic attraction or
repulsion.
K: Constant, whose value depends
on the system of units.
u: magnetic permeability. It has
no units and its value depends on the medium in which the magnetic poles are
located.
m: Intensity of the magnetic poles
or magnetic mass.
d: distance between external
magnetic poles.
Units:
Magnetic constant ( μo )
The coefficient "K" in
the international system can be written as:
The magnitude μo is called the magnetic
constant and its value is:
Unit of Magnetic Pole Strenght
Amper x meter (A.m):
In the International System it is
defined as the magnetic mass that acting upon another like it in the vacuum and
with one meter of distance, they repel each other with a force of 10-7N.
[Magnetic mass] = [A.m]
The magnetic permeability in the
vacuum is equal to unity (μ=1) and in the air has approximately the same
value.
MAGNETIC FIELD
CONCEPT
It is a property of matter as a
result of moving electric charges (electric current). The magnetic field is the
geometric place where the magnet affects with their magnetic effects on another
object with magnetic mass or on moving electric charges. In that sense the
magnetic field exerts its force (F).
Notably, the magnetic field is a
vector field thus a vector quantity associated with each point in space. To
represent the magnetic field the symbol B is used.
LINES OF FORCE
They are such geometric lines that
serve to represent graphically the magnetic field. In a magnet the lines of
force emerge from the north pole (N) and enter the south pole (S); the latter
is done by convention.
The magnetic force F that acts
over a positive charge, moves with velocity v and is perpendicular to the magnetic field B and
v. The force is greater when v and B are perpendicular.
a) Given a charge moving parallel
to the magnetic field experiences a zero magnetic force.
b) If a charge moves at an angle θ with respect to a magnetic field, it will experience a magnetic force of
magnitude:
Note that F is perpendicular to the plane
containing
c) If a charge moves perpendicular
to a magnetic field, it will experience a high magnetic force with magnitude
Calculating the direction of the
magnetic force on a moving charged particle.
a) The right hand rule for the
direction of the magnetic force on a positive charge moving in a magnetic
field:
- Place v and B in such a way that
they were attached to their origins.
- Imagine that v is turned to B in
the v-B plane.
- The force acts along a line that
is perpendicular to the plane v-B.
Gyrate the fingers of the right hand around
the line. In that sense, the thumb points in the same way as the acting force.
b) If the charge is negative, then
the direction of the force is opposite to the one made with the right hand
rule.
The unit of the International
System for B is equal to 1 ns / cm, due to the fact that one ampere is a
Coulomb per second (1 A = 1C / s), 1N / Am. This unit is called tesla (T):
1 Tesla = 1 T = 1 N / a.m
* The instruments used to measure
magnetic fields sometimes are called Gaussmeters. A gauss (1G = 10-4 T) is
another unit B that is also commonly used.
* The magnetic field of the earth
is approximately 10-4T, ie, 1G.
* Inside the atoms are magnetic
fields of the order of 10T, which are of great importance in the analysis of
atomic spectra.
* It is likely that the magnetic
field on the surface of a neutron star is about 108
T.
MAGNETIC FIELD STRENGTH (H)
It is a vector physical quantity
used to describe the magnetic field. Its value is defined as the resultant
magnetic force acting per each unit mass at a point in a magnetic field.
The vector intensity of the
magnetic field has the same direction of the resultant magnetic force.
Where:
M: Magnetic mass north or south,
creator of the magnetic field.
m: Magnetic mass north, the
magnetic field detector.
From the quantitative law, the
value of the force is replaced and we obtain.
Representation of the magnetic field strength
The tangent to the line of
magnetic force has the same direction of the vector magnetic field strength at
that point and is unique, therefore, the lines of forces are not cut.
H1: Due to North Pole
H2: Due to South Pole
mo: North test. Magnetic mass.
H = H1 + H2
In the case of a magnet, their
north and south magnetic masses are equal.
Mnorth= Msouth = M
Pair of forces on a bar magnet in
an external magnetic field where a force on the north pole and the other on the
south pole origins, equal in magnitude and opposite in direction, that tend to
align with the external uniform magnetic field, forming a couple of forces
whose value is equal to the product of one of the forces multiplied by the
perpendicular distance between the forces.
* Cupla: couple of forces
Cupla = C = F. D Seno
MAGNETIC FLUX (ϕ)
It is defined as the product of
magnetic field strength H and the surface A perpendicular to the lines of force
of the field.
ϕ=H.A
Where ϕ is the number of lines
of force.
If the surface was inclined to the
lines of force, then according to the graph:
ϕ =H.A.Cosθ
The magnetic flux in the International System (SI) is measured in "weber". The unit of the SI for the magnetic flux is equal to the unit of magnetic field (1T) multiplied by the unit area (1m2).
Observation:
* It should be noted that the
magnetic field lines never have endpoints, unlike the electric field lines that
begin and end in electrical charges. Although it appears that the magnetic
field lines start at the north pole and terminate at the south pole, actually
the field lines of a magnet pass through its interior.
Magnetic induction (B)
Also called magnetic flux density.
It is that vector that is used to write the magnetic field. Its value is
defined as the number of lines of force that perpendicularly cross through the
unit area of a surface located in the magnetic field.
If θ = 0⁰ then the lines of force
are perpendicular to the surface.
Magnetic Permeability (μ)
It is a dimensionless magnitude
and its value indicates the behavior that experiences a substance when it is
located within an external magnetic field. In that sense, the magnetic
permeability indicates if the dispersed substance concentrates or not alter the
magnetic field or the lines of force.
It is defined as the quotient of
the magnetic induction (B) and the magnetic field intensity in the vacuum.
1. Paramagnetic Substance (μ ≥1):
They are those substances that
when being inside a magnetic field weakly concentrate the lines of force or
they just don't alter them. This type of substance has constant magnetic
permeability slightly greater or equal to unity. Examples are aluminum,
platinum, air, vacuum, etc.
2. Diamagnetic Substances (μ <1):
They are those substances that
disperse the lines of force in an external magnetic field, so that they
magnetize in an opposite sense to the inductor magnetic field. Such a substance
has constant magnetic permeability and its value is less than one. Examples of
them are antimony, bismuth, water, etc.
3. Ferromagnetic Substance (μ >1):
They are such substances that in
an external magnetic field concentrate the lines of force, so that they
magnetize for the inductor magnetic field.
These substances have varying
magnetic permeability much greater than the value of one. Examples are iron,
nickel, cobalt, etc.
Illustrative examples
1.
A particle of mass m and charge q enters a square region where there is a magnetic field perpendicular to the region, with a
velocity 18x104m/s. If q/m = 0,18x 1012
C / kg. For which side of the
region the particle scapes?
If
B=1G=10-4 T
Then:
By plotting the path of the particle is obtained:
In that sense, the particle scapes by the side GF
2. An electron inside a particle accelerator obtains a kinetic energy of 239.1 keV. It enters perpendicularly to an uniform magnetic field with 0,4T. What is the radius (in mm) of the resulting circular path?
me= 9,1 x 10-31kg
We know that:
Then:
1ev= 1,16 x 10-19 J
B = 0,4 T
Ec = 239,1 Kev
We also have that:
In that sense, the radius of the resulting circular path is 4,1 mm
3. The magnet is attached by a rope ab from one of the magnetic poles. The intensity of each pole of the magnet is equal to 3A.m and its weight is W = 24N. If the system is within an external magnetic field, uniform and horizontal with Intensity M = 4 (A / m) and the figure shows a magnet bar in equilibrium. Find the angle theta which define the equilibrium position.
When applying the second condition
of equilibrium with respect to point A.
4. Determine the intensity of the magnetic field generated by a bar magnet in the points of the circumference shown. The separation distance between the magnetic poles is "2a", and the magnetic masses of the north and south poles are equals to "m". The value of magnetic intensity should be expressed in terms of angle θ.
From the graph:
Then:
INTERESTING NEWS ABOUT MAGNETISM
JAPAN’S MAGLEV TRAIN HAS BROKEN WORLD SPEED RECORDS BY HITTING 603 KM/H
The experimental train called Maglev broke records by hitting 603 km/h (374 mph). This train runs on magnets rather than wheels. It works with the principle that when magnets are pushed together (north/north) or (south/south), they repel each other.
The Maglevs (Magnetic Levitation trains) have magnets in the bottom and they are repelled from the track below that is also magnetic, then the train floats 10 cm above the ground so that there is much less friction, hence it can reach such great speeds.
BBC (2015, April 21). newsbeat. Japan's Maglev: Slower than a bullet, faster than wind. Retrieved from http://www.bbc.co.uk/newsbeat/article/32393166/japans-maglev-slower-than-a-bullet-faster-than-wind