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Magnetic fields
By: The University of Faisalabad
Magnets
 All magnets attract iron, such as that in a refrigerator door. However, magnets may
attract or repel other magnets.
 Experimentation shows that all magnets have two poles. If freely suspended, one
pole will point toward the north.
 The two poles are thus named the north magnetic pole and the south magnetic
pole.
 It is a universal characteristic of all magnets that like poles repel and unlike
poles attract.
Magnetic Fields
 Einstein is said to have been fascinated by a compass as a child, perhaps musing
on how the needle felt a force without direct physical contact.
 His ability to think deeply and clearly about action at a distance, particularly for
gravitational, electric, and magnetic forces, later enabled him to create his
revolutionary theory of relativity.
 Since magnetic forces act at a distance, we define a magnetic field to represent
magnetic forces.
Magnetic Fields
 The pictorial representation of magnetic field lines is very useful in visualizing the
strength and direction of the magnetic field.
 The direction of magnetic field lines is defined to be the direction in which the
north end of a compass needle points. The magnetic field is traditionally called the
B-field.
 A field is a way of mapping forces surrounding any object that can act on another
object at a distance without apparent physical connection. The field represents the
object generating it. Gravitational fields map gravitational forces, electric fields map
electrical forces, and magnetic fields map magnetic forces.
Properties of magnetic field lines
1. The direction of the magnetic field is tangent to the field line at any point in space.
A small compass will point in the direction of the field line.
2. The strength of the field is proportional to the closeness of the lines. It is exactly
proportional to the number of lines per unit area perpendicular to the lines (called
the areal density).
3. Magnetic field lines can never cross, meaning that the field is unique at any point
in space.
4. Magnetic field lines are continuous, forming closed loops without beginning or end.
They go from the north pole to the south pole.
Force on a Moving Charge in a
Magnetic Field
 What is the mechanism by which one magnet exerts a force on another? The
answer is related to the fact that all magnetism is caused by current, the flow of
charge.
 Magnetic fields exert forces on moving charges, and so they exert forces on other
magnets, all of which have moving charges.
Right Hand Rule
 The magnetic force on a moving charge is one of the most fundamental known.
 Magnetic force is as important as the electrostatic or Coulomb force.
 Yet the magnetic force is more complex, in both the number of factors that affects it
and in its direction, than the relatively simple Coulomb force.
 Themagnitude of the magnetic force F on a charge q moving at a speed v in a
magnetic field of strength B is given by
𝐹 = 𝑞𝑣𝐵 sin 𝜃
Right Hand Rule
 where θ is the angle between the directions of v and B.
 This force is often called the Lorentz force. In fact, this
is how we define the magnetic field strength B —in terms
of the force on a charged particle moving in a magnetic
field.
 The SI unit for magnetic field strength B is called the
tesla (T)
𝐵 =
𝐹
𝑞𝑣 sin 𝜃
 The direction of the magnetic force F is perpendicular to
the plane formed by v and B , as determined by the
right hand rule.
Force on a Moving Charge in a
Magnetic Field
 Magnetic force can cause a charged particle to move in a circular or spiral path.
 Cosmic rays are energetic charged particles in outer space, some of which
approach the Earth. They can be forced into spiral paths by the Earth’s magnetic
field.
 Protons in giant accelerators are kept in a circular path by magnetic force.
 The curved paths of charged particles in magnetic fields are the basis of a number
of phenomena and can even be used analytically, such as in a mass spectrometer.
Force on a Moving Charge in a
Magnetic Field
 So does the magnetic force cause circular motion?
 Magnetic force is always perpendicular to velocity, so that it does no work on the
charged particle.
 The particle’s kinetic energy and speed thus remain constant.
 The direction of motion is affected, but not the speed.
 This is typical of uniform circular motion.
 The magnetic force supplies the centripetal force
𝐹𝑐 =
𝑚𝑣2
𝑟
Noting that sin θ = 1 , we see that F = qvB
 A negatively charged particle
moves in the plane of the page in
a region where the magnetic field
is perpendicular into the page
 The magnetic force is
perpendicular to the velocity, and
so velocity changes in direction
but not magnitude. Uniform
circular motion results.
Force on a Moving Charge in a
Magnetic Field
𝑞𝑣𝐵 =
𝑚𝑣2
𝑟
𝑟 =
𝑚𝑣
𝑞𝐵
 Here, r is the radius of curvature of the path of a charged particle with mass m and
charge q , moving at a speed v perpendicular to a magnetic field of strength B .
 If the velocity is not perpendicular to the magnetic field, then v is the component of
the velocity perpendicular to the field.
 Thecomponent of the velocity parallel to the field is unaffected, since the magnetic
force is zero for motion parallel to the field.
 This produces a spiral motion rather than a circular one.
The Hall Effect
 We have seen effects of a magnetic field on free-moving charges. The magnetic
field also affects charges moving in a conductor. One result is the Hall effect,
The Hall effect
 The field is perpendicular to the electron drift velocity and to the width of the
conductor.
 Note that conventional current is to the right in both parts of the figure. In part
(a), electrons carry the current and move to the left.
(b), positive charges carry the current and move to the right.
 Moving electrons feel a magnetic force toward one side of the conductor, leaving a
net positive charge on the other side. This separation of charge creates a voltage ε
, known as the Hall emf, across the conductor.
 The creation of a voltage across a current carrying conductor by a magnetic field is
known as the Hall effect,
Numerical
A Hall effect flow probe is placed on an artery, applying a
0.100-T magnetic field across it. What is the Hall emf,
given the vessel’s inside diameter is 4.00 mm and the
average blood velocity is 20.0 cm/s?

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Magnetic fields

  • 1. Magnetic fields By: The University of Faisalabad
  • 2. Magnets  All magnets attract iron, such as that in a refrigerator door. However, magnets may attract or repel other magnets.  Experimentation shows that all magnets have two poles. If freely suspended, one pole will point toward the north.  The two poles are thus named the north magnetic pole and the south magnetic pole.  It is a universal characteristic of all magnets that like poles repel and unlike poles attract.
  • 3. Magnetic Fields  Einstein is said to have been fascinated by a compass as a child, perhaps musing on how the needle felt a force without direct physical contact.  His ability to think deeply and clearly about action at a distance, particularly for gravitational, electric, and magnetic forces, later enabled him to create his revolutionary theory of relativity.  Since magnetic forces act at a distance, we define a magnetic field to represent magnetic forces.
  • 4. Magnetic Fields  The pictorial representation of magnetic field lines is very useful in visualizing the strength and direction of the magnetic field.  The direction of magnetic field lines is defined to be the direction in which the north end of a compass needle points. The magnetic field is traditionally called the B-field.  A field is a way of mapping forces surrounding any object that can act on another object at a distance without apparent physical connection. The field represents the object generating it. Gravitational fields map gravitational forces, electric fields map electrical forces, and magnetic fields map magnetic forces.
  • 5. Properties of magnetic field lines 1. The direction of the magnetic field is tangent to the field line at any point in space. A small compass will point in the direction of the field line. 2. The strength of the field is proportional to the closeness of the lines. It is exactly proportional to the number of lines per unit area perpendicular to the lines (called the areal density). 3. Magnetic field lines can never cross, meaning that the field is unique at any point in space. 4. Magnetic field lines are continuous, forming closed loops without beginning or end. They go from the north pole to the south pole.
  • 6. Force on a Moving Charge in a Magnetic Field  What is the mechanism by which one magnet exerts a force on another? The answer is related to the fact that all magnetism is caused by current, the flow of charge.  Magnetic fields exert forces on moving charges, and so they exert forces on other magnets, all of which have moving charges.
  • 7. Right Hand Rule  The magnetic force on a moving charge is one of the most fundamental known.  Magnetic force is as important as the electrostatic or Coulomb force.  Yet the magnetic force is more complex, in both the number of factors that affects it and in its direction, than the relatively simple Coulomb force.  Themagnitude of the magnetic force F on a charge q moving at a speed v in a magnetic field of strength B is given by 𝐹 = 𝑞𝑣𝐵 sin 𝜃
  • 8. Right Hand Rule  where θ is the angle between the directions of v and B.  This force is often called the Lorentz force. In fact, this is how we define the magnetic field strength B —in terms of the force on a charged particle moving in a magnetic field.  The SI unit for magnetic field strength B is called the tesla (T) 𝐵 = 𝐹 𝑞𝑣 sin 𝜃  The direction of the magnetic force F is perpendicular to the plane formed by v and B , as determined by the right hand rule.
  • 9. Force on a Moving Charge in a Magnetic Field  Magnetic force can cause a charged particle to move in a circular or spiral path.  Cosmic rays are energetic charged particles in outer space, some of which approach the Earth. They can be forced into spiral paths by the Earth’s magnetic field.  Protons in giant accelerators are kept in a circular path by magnetic force.  The curved paths of charged particles in magnetic fields are the basis of a number of phenomena and can even be used analytically, such as in a mass spectrometer.
  • 10. Force on a Moving Charge in a Magnetic Field  So does the magnetic force cause circular motion?  Magnetic force is always perpendicular to velocity, so that it does no work on the charged particle.  The particle’s kinetic energy and speed thus remain constant.  The direction of motion is affected, but not the speed.  This is typical of uniform circular motion.  The magnetic force supplies the centripetal force 𝐹𝑐 = 𝑚𝑣2 𝑟 Noting that sin θ = 1 , we see that F = qvB
  • 11.  A negatively charged particle moves in the plane of the page in a region where the magnetic field is perpendicular into the page  The magnetic force is perpendicular to the velocity, and so velocity changes in direction but not magnitude. Uniform circular motion results.
  • 12. Force on a Moving Charge in a Magnetic Field 𝑞𝑣𝐵 = 𝑚𝑣2 𝑟 𝑟 = 𝑚𝑣 𝑞𝐵  Here, r is the radius of curvature of the path of a charged particle with mass m and charge q , moving at a speed v perpendicular to a magnetic field of strength B .  If the velocity is not perpendicular to the magnetic field, then v is the component of the velocity perpendicular to the field.  Thecomponent of the velocity parallel to the field is unaffected, since the magnetic force is zero for motion parallel to the field.  This produces a spiral motion rather than a circular one.
  • 13. The Hall Effect  We have seen effects of a magnetic field on free-moving charges. The magnetic field also affects charges moving in a conductor. One result is the Hall effect,
  • 14. The Hall effect  The field is perpendicular to the electron drift velocity and to the width of the conductor.  Note that conventional current is to the right in both parts of the figure. In part (a), electrons carry the current and move to the left. (b), positive charges carry the current and move to the right.  Moving electrons feel a magnetic force toward one side of the conductor, leaving a net positive charge on the other side. This separation of charge creates a voltage ε , known as the Hall emf, across the conductor.  The creation of a voltage across a current carrying conductor by a magnetic field is known as the Hall effect,
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  • 16. Numerical A Hall effect flow probe is placed on an artery, applying a 0.100-T magnetic field across it. What is the Hall emf, given the vessel’s inside diameter is 4.00 mm and the average blood velocity is 20.0 cm/s?