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The Field Of a
Magnetized Object
INTRODUCTION TO
ELECTRODYNAMICS
Submitted to : Ma’am Ammara
Submitted by : Group-3
B.S Physics (5th Semester)
Section (A)
GCWU Sialkot
Group Members:
• Bisma Shakir 14020210-018
• Faiqa Barkat 14020210-027
• Maria Kousar 14020210-005
•Maham Idrees 14020210-010
•Warda Jabbar 14020210-048
•Ishrat Fardoos 14020210-012
•Nimra Asmat 14020210-021
CONTENTS:
 Magnetization
 Dia-magnetism
 Para-magnetism
 Fero-magnetism
The Field Of A Magnetized Object
Magnetization:
Definition:
“The process of making a substance
temporarily or permanently magnetic, as by
insertion in a magnetic field.”
“OR”
“The extent to which an object is magnetized”
M = magnetic dipole moment per unit
volume.
Dia-magnetism:
“ Diamagnetic materials acquire a very
weak magnetization opposite an external applied
magnetic field, and lose their alignment when the field
is removed. ”
Examples:
Bi, Zn, Gold, H2O, Alkali Earth elements (Be,
Mg, Ca, Sr)
Cont…
Properties of dia-magnetism:
• They are repelled by the external applied magnetic field.
• The permanent dipoles are absent in diamagnetic
materials.
• In a non-uniform magnetic field, they are repelled away
from the stronger parts of the field.
• The relative permeability ( µr ) is always less than one.
Paramagnetism:
“ Paramagnetic materials acquire a weak
magnetization aligned with an external applied
magnetic field , and also lose their magnetization
when the field is removed.”
Examples:
Alkali Metals ( Li, Na, K,Rb ) , Transition
Metals , Al , Pt , Mn , Cr etc
Cont…
Properties of paramagnetism:
• Paramagnetic materials experience a feeble
attractive force when brought near the pole of a
magnet.
• There materials possess some permanent dipole
moment which arise due to some unpaired
electrons.
• The magnetic susceptibility is small and +ve.
Ferromagnetism:
“ They have dipoles which can align with an
external magnetic field to produce a much
stronger magnetization, and also they retain the
magnetization after the field is removed. ”
Examples:
Fe , Co , Ni etc.
Cont…
Properties of ferromagnetism:
• The direction in which the material gets magnetised is
the same as that of the external field.
• These materials exhibits magnetization even in the
absence of an external magnetic field . This property is
called spontaneous magnetization.
• Ferromagnetic materials experience a very strong
attractive force when brought near the pole of a magnet.
• Permeability is very much greater than one.
• Susceptibility is +ve and high.
Field Of A Magnetized Object:
Bound Currents:
• Suppose we have a piece of magnetized material ; the
magnetic dipole moment per unit volume , M is given.
• Starting with the vector potential of an ideal dipole at the
origin:
• we can write this more generally as the potential when the
dipole is at position r’ :
Cont…
• Then if m= M(r’) we can get the potential due to a
distribution of magnetic dipoles as :
• For pretty well any configuration, this integral is difficult or
impossible to calculate analytically, but we can transform it
into a different form, in a similar way to that used in the
electrostatic case for polarization.
Cont…
• First , we use the formula :
• So potential becomes:
Cont…
• Now we can use a vector product rule:
• By using f = 1/(r-r’) and V = M we get equation as:
Cont…
• The first integral looks like the potential of a volume
current density :
• So equation no.7 becomes:
Cont…
• The second integral can be transformed into a surface
integral by using the divergence theorem.
• For a general vector field “V” and a constant vector
field “C” we have, using a vector identity in the first line:
Cont…
Thus,
Cont…
• So , equation 9 becomes :
• If we now define a surface current :
• where nˆ is the unit normal to the surface.
Cont…
• So, with these functions , we have the final relation:
• This means that the potential of a magnetized object is the same as
would be produced by a volume current throughout
the material, plus a surface current on the boundary.
Bibliography:
• http://unlcms.unl.edu/cas/physics/tsymbal/teaching/E
M-913/section6-Magnetostatics.pdf
• http://www.physicspages.com/2013/06/29/magnetizati
on-bound-currents/
• http://www.slideshare.net/9998366697/diamagnetism
paramagnetismferromagnetismantiferromagnetism-
and-ferrimagnetismmagnetic-materials-
ppt?qid=05467164-ae00-48fa-bf8c-
595ea584a4be&v=&b=&from_search=4
field of a magnetized object

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field of a magnetized object

  • 1.
  • 2. The Field Of a Magnetized Object INTRODUCTION TO ELECTRODYNAMICS
  • 3. Submitted to : Ma’am Ammara Submitted by : Group-3 B.S Physics (5th Semester) Section (A) GCWU Sialkot Group Members: • Bisma Shakir 14020210-018 • Faiqa Barkat 14020210-027 • Maria Kousar 14020210-005 •Maham Idrees 14020210-010 •Warda Jabbar 14020210-048 •Ishrat Fardoos 14020210-012 •Nimra Asmat 14020210-021
  • 4. CONTENTS:  Magnetization  Dia-magnetism  Para-magnetism  Fero-magnetism The Field Of A Magnetized Object
  • 5. Magnetization: Definition: “The process of making a substance temporarily or permanently magnetic, as by insertion in a magnetic field.” “OR” “The extent to which an object is magnetized” M = magnetic dipole moment per unit volume.
  • 6. Dia-magnetism: “ Diamagnetic materials acquire a very weak magnetization opposite an external applied magnetic field, and lose their alignment when the field is removed. ” Examples: Bi, Zn, Gold, H2O, Alkali Earth elements (Be, Mg, Ca, Sr)
  • 8. Properties of dia-magnetism: • They are repelled by the external applied magnetic field. • The permanent dipoles are absent in diamagnetic materials. • In a non-uniform magnetic field, they are repelled away from the stronger parts of the field. • The relative permeability ( µr ) is always less than one.
  • 9. Paramagnetism: “ Paramagnetic materials acquire a weak magnetization aligned with an external applied magnetic field , and also lose their magnetization when the field is removed.” Examples: Alkali Metals ( Li, Na, K,Rb ) , Transition Metals , Al , Pt , Mn , Cr etc
  • 11. Properties of paramagnetism: • Paramagnetic materials experience a feeble attractive force when brought near the pole of a magnet. • There materials possess some permanent dipole moment which arise due to some unpaired electrons. • The magnetic susceptibility is small and +ve.
  • 12. Ferromagnetism: “ They have dipoles which can align with an external magnetic field to produce a much stronger magnetization, and also they retain the magnetization after the field is removed. ” Examples: Fe , Co , Ni etc.
  • 14. Properties of ferromagnetism: • The direction in which the material gets magnetised is the same as that of the external field. • These materials exhibits magnetization even in the absence of an external magnetic field . This property is called spontaneous magnetization. • Ferromagnetic materials experience a very strong attractive force when brought near the pole of a magnet. • Permeability is very much greater than one. • Susceptibility is +ve and high.
  • 15. Field Of A Magnetized Object: Bound Currents: • Suppose we have a piece of magnetized material ; the magnetic dipole moment per unit volume , M is given. • Starting with the vector potential of an ideal dipole at the origin: • we can write this more generally as the potential when the dipole is at position r’ :
  • 16.
  • 17. Cont… • Then if m= M(r’) we can get the potential due to a distribution of magnetic dipoles as : • For pretty well any configuration, this integral is difficult or impossible to calculate analytically, but we can transform it into a different form, in a similar way to that used in the electrostatic case for polarization.
  • 18. Cont… • First , we use the formula : • So potential becomes:
  • 19. Cont… • Now we can use a vector product rule: • By using f = 1/(r-r’) and V = M we get equation as:
  • 20. Cont… • The first integral looks like the potential of a volume current density : • So equation no.7 becomes:
  • 21. Cont… • The second integral can be transformed into a surface integral by using the divergence theorem. • For a general vector field “V” and a constant vector field “C” we have, using a vector identity in the first line:
  • 23. Cont… • So , equation 9 becomes : • If we now define a surface current : • where nˆ is the unit normal to the surface.
  • 24. Cont… • So, with these functions , we have the final relation: • This means that the potential of a magnetized object is the same as would be produced by a volume current throughout the material, plus a surface current on the boundary.
  • 25. Bibliography: • http://unlcms.unl.edu/cas/physics/tsymbal/teaching/E M-913/section6-Magnetostatics.pdf • http://www.physicspages.com/2013/06/29/magnetizati on-bound-currents/ • http://www.slideshare.net/9998366697/diamagnetism paramagnetismferromagnetismantiferromagnetism- and-ferrimagnetismmagnetic-materials- ppt?qid=05467164-ae00-48fa-bf8c- 595ea584a4be&v=&b=&from_search=4