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Electric dipoles are fundamental to understanding distribution in molecules and materials. They arise from the separation of positive and negative charges, creating a that interacts with electric fields.

Permanent dipoles exist in asymmetric molecules like water, while induced dipoles form in neutral atoms exposed to external fields. These concepts are crucial for grasping how materials respond to electric fields and interact with each other.

Electric Dipoles

Permanent electric dipoles in molecules

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  • System with two equal and opposite charges separated by a fixed distance charges not free to move independently
  • (p\vec{p}) vector quantity characterizes strength and orientation of dipole p=qd\vec{p} = q\vec{d}, qq magnitude of each charge, d\vec{d} from negative to positive charge
  • Many molecules have due to asymmetric structure and
    • In water, oxygen atom attracts electrons more strongly than hydrogen atoms creates charge separation
    • Bent geometry of water molecule results in net dipole moment
  • plays a crucial role in determining the presence and strength of permanent dipoles

Formation of induced electric dipoles

  • Induced occurs when neutral atom or molecule subjected to external electric field causes redistribution of electron cloud creates charge separation
  • Positive charges (nuclei) slightly displaced in direction of electric field, negative charges (electrons) displaced in opposite direction
  • Magnitude of moment depends on strength of external electric field and of atom or molecule polarizability measures how easily electron cloud can be distorted by external field
  • Induced dipoles are temporary exist only in presence of external electric field
  • Polarization occurs when many molecules in a material align their dipoles in response to an external electric field

Calculation of electric dipole moment

  • moment (p\vec{p}) calculated using formula p=qd\vec{p} = q\vec{d}
    • qq magnitude of each charge in dipole
    • d\vec{d} displacement vector from negative to positive charge
  • SI unit for electric dipole moment (C·m)
  • Larger dipole moment indicates stronger charge separation more significant effect on surrounding electric field
  • (UU) of electric dipole in external electric field (E\vec{E}) given by U=pEU = -\vec{p} \cdot \vec{E} dipole tends to align itself with electric field to minimize potential energy
  • (τ\vec{\tau}) experienced by electric dipole in external electric field given by τ=p×E\vec{\tau} = \vec{p} \times \vec{E} causes dipole to rotate and align with field

Behavior of dipoles in electric fields

  • In , electric dipole experiences only torque no net force
    • Torque causes dipole to rotate and align with field
    • Once aligned, dipole remains in stable equilibrium
  • In , electric dipole experiences both torque and net force
    • Net force directed towards region of higher electric field strength
    • Phenomenon known as
  • Force on electric dipole in non-uniform electric field given by F=(p)E\vec{F} = (\vec{p} \cdot \nabla)\vec{E}
    • \nabla represents rate of change of electric field in space
  • Behavior of electric dipoles in non-uniform fields basis for various applications in microfluidics and particle manipulation

Dipoles in materials and electrostatics

  • Dielectric constant measures a material's ability to store electrical energy in an electric field, related to its molecular dipole properties
  • studies the behavior of stationary electric charges and fields, including the effects of electric dipoles
  • occur between molecules with permanent or induced dipoles, influencing material properties and behavior
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© 2024 Fiveable Inc. All rights reserved.
AP® and SAT® are trademarks registered by the College Board, which is not affiliated with, and does not endorse this website.

© 2024 Fiveable Inc. All rights reserved.
AP® and SAT® are trademarks registered by the College Board, which is not affiliated with, and does not endorse this website.
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