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Electric Fields in Matter Polarization Electric displacement Field of a polarized object Linear dielectrics
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Matter Insulators/Dielectrics Conductors All charges are attached to specific atoms/molecules and can only have a restricted motion WITHIN the atom/molecule.
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When a neutral atom is placed in an external electric field (E): … positively charged core ( nucleus) is pushed along E; If E is large enough ► the atom gets pulled apart completely => the atom gets IONIZED … centre of the negatively charged cloud is pushed in the opposite direction of E;
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For less extreme fields ► an equilibrium is established => the atom gets POLARIZED ……. the attraction between the nucleus and the electrons AND ……. the repulsion between them caused by E
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Induced Dipole Moment: Atomic Polarizability (pointing along E)
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To calculate : (in a simplified model) The model: an atom consists of a point charge (+q) surrounded by a uniformly charged spherical cloud of charge (-q). At equilibrium, ( produced by the negative charge cloud) -q E d +q a -q
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At distance d from centre, (where v is the volume of the atom)
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Prob. 4.4: A point charge q is situated a large distance r from a neutral atom of polarizability . Find the force of attraction between them. Force on q :
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Alignment of Polar Molecules: when put in a uniform external field: Polar molecules: molecules having permanent dipole moment
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Alignment of Polar Molecules: when put in a non-uniform external field: d F+F+ F-F- -q +q
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F-F- d F+F+ -q +q E+E+ E-E-
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For perfect dipole of infinitesimal length, the torque about the centre : the torque about any other point:
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Prob. 4.9: A dipole p is a distance r from a point charge q, and oriented so that p makes an angle with the vector r from q to p. (i) What is the force on p? (ii) What is the force on q?
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Polarization: When a dielectric material is put in an external field: A lot of tiny dipoles pointing along the direction of the field Induced dipoles (for non-polar constituents) Aligned dipoles (for polar constituents)
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A measure of this effect is POLARIZATION defined as: P dipole moment per unit volume Material becomes POLARIZED
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The Field of a Polarized Object = sum of the fields produced by infinitesimal dipoles p rsrs
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Dividing the whole object into small elements, the dipole moment in each volume element d ’ : Total potential :
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Prove it ! Use a product rule :
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Using Divergence theorem;
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Defining: Volume Bound Charge Surface Bound Charge
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surface charge density b volume charge density b
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Field/Potential of a polarized object Field/Potential produced by a surface bound charge b Field/Potential produced by a volume bound charge b + =
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Physical Interpretation of Bound Charges …… are not only mathematical entities devised for calculation; perfectly genuine accumulations of charge ! but represent
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-q +q d A Surface Bound Charge A dielectric tube Dipole moment of the small piece: = Surface charge density: P
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A P A’ In general: If the cut is not to P :
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+ + + + + + + + _ _ _ _ _ _ _ __ Volume Bound Charge A non-uniform polarization accumulation of bound charge within the volume diverging P pile-up of negative charge
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Net accumulated charge with a volume Opposite to the amount of charge pushed out of the volume through the surface =
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Field of a uniformly polarized sphere Choose: z-axis || P P is uniform z PR
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Potential of a uniformly polarized sphere: (Prob. 4.12) Potential of a polarized sphere at a field point ( r ): P is uniform P is constant in each volume element
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Electric field of a uniformly charged sphere
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At a point inside the sphere ( r < R )
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Inside the sphere the field is uniform
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At a point outside the sphere ( r > R )
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(potential due to a dipole at the origin) Total dipole moment of the sphere:
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Uniformly polarized sphere – A physical analysis Without polarization: Two spheres of opposite charge, superimposed and canceling each other With polarization: The centers get separated, with the positive sphere moving slightly upward and the negative sphere slightly downward
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At the top a cap of LEFTOVER positive charge and at the bottom a cap of negative charge Bound Surface Charge b + + + + + +-+- d + + - - - - - -
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Recall: Pr. 2.18 Two spheres, each of radius R, overlap partially. ++ -- _ + d _ +
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Electric field in the region of overlap between the two spheres + + + + + +-+- d + + - - - - - - For an outside point:
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Prob. 4.10: A sphere of radius R carries a polarization where k is a constant and r is the vector from the center. (i) Calculate the bound charges b and b. (ii) Find the field inside and outside the sphere.
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The Electric Displacement Polarization Accumulation of Bound charges Total field = Field due to bound charges + field due to free charges
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Gauss’ Law in the presence of dielectrics Within the dielectric the total charge density: bound charge free charge caused by polarization NOT a result of polarization
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Gauss’ Law : Electric Displacement ( D ) :
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Gauss’ Law
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D & E :
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Boundary Conditions: On normal components: On tangential components:
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For some material (if E is not TOO strong) Electric susceptibility of the medium Linear Dielectrics Recall: Cause of polarization is an Electric field Total field due to (bound + free) charges
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Location ► Homogeneous Magnitude of E ► Linear Direction of E ► Isotropic In a dielectric material, if e is independent of :
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In linear (& isotropic) dielectrics; Permittivity of the material The dimensionless quantity: Relative permittivity or Dielectric constant of the material
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and / or Electric Constitutive Relations Represent the behavior of materials
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But in a homogeneous linear dielectric : Generally, even in linear dielectrics :
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When the medium is filled with a homogeneous linear dielectric, the field is reduced by a factor of 1/ r.
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Capacitor filled with insulating material of dielectric constant r :
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Energy in Dielectric Systems Recall: The energy stored in any electrostatic system: The energy stored in a linear dielectric system:
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