Interaction of Charged Objects traction: can happen also for like-charged objects! pulsion: can happen only for like-charged objects! Intervening matter does not “block” the E field The resulting field is a superposition of two fields: Field of the charge plus the field of induced dipoles. + - +
Interaction of Charged Objects. Repulsion: can happen only for like-charged objects!. Attraction: can happen also for like-charged objects!. Intervening matter does not “ block ” the E field. The resulting field is a superposition of two fields : - PowerPoint PPT Presentation
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Interaction of Charged Objects
Attraction: can happen also for like-charged objects!
Repulsion: can happen only for like-charged objects!
Intervening matter does not “block” the E field
The resulting field is a superposition of two fields: Field of the charge plus the field of induced dipoles.
+ - +
Clicker QuestionA
B D
C
What is the direction of the electric field at X due to the dipole?
Clicker QuestionA
B D
C
What is the direction of the electric field at X due to the plastic block?
Clicker QuestionA
B D
C
What is the direction of the NET electric field at X?
Clicker Question
The force of one of the permanent dipoles on the other is:
A) AttractiveB) RepulsiveC) The force is zero
Different materials respond differently to electric field
Conductor: contains mobile charges that can move through material
Insulator: contains no mobile charges
Conductors and Insulators
Insulator: Electrons are bound to the atoms or molecules.
Electrons can shift slightly (<1 Å), but remain bound to the molecule.
Individual atoms or molecules can be polarized by external electric field.
There are a lot of molecules – the net effect produced by the induced dipoles can be very large.
Polarization of Insulators
Diagram showing polarization of an insulator:
Dipoles: exaggerated in size; stretch: degree of polarization
No mobile charges: excess charges stay where they are
Polarization of Insulators
Field E at a location of a molecule is a superposition of the external applied field and the field created by other induced dipoles:
Simplifying assumption:
Low Density Approximation
There are charges which can move freely throughout the material
E
In contrast to an insulator, where electrons and nuclei can move only very small distances, the charged particles in a conductor are free to move large distances.Polarization of conductors differs from that of insulators.
Conductors
Salt water:Na+ and Cl-
H+ and OH-
Apply externalelectric field
Ionic Solutions are Conductors
When an electric field is applied to a conductor, the mobile charged particles begin to move in the direction of the force exerted on them by the field.
As the charges move, they begin to pile up in one location, creating a concentration of charge creates electric field.
The net electric field is the superposition of the applied field and field created by the relocated charges.
Assumption: charges will move until Enet=0 (static equilibrium)
It is not a shielding effect, but a consequence of superposition!
Proof: by contradiction:
Mobile ions will move
This is not equilibrium
Assume Enet≠0
Assumption Enet≠0 is wrong
Enet=0
Ionic Solutions are Conductors
Positive atomic coresand mobile-electron sea
Electrons are not completely free – they are bound to the metal as a whole.
Metal lattice
There is no net interaction between mobile electrons
A Model of a Metal
We will return to this idea when we discuss the force on a current carrying wire in a magnetic field.
Simplified diagram of polarized metal
Note: It is not charged!Net charge is still zero
Metal in Electric Field
In static equilibrium:
Enet= 0 everywhere inside the metal!
Mobile charges on surface rearrange to achieve Enet= 0 Actual arrangement might be very complex!It is a consequence of 1/r2 distance dependence
Enet= 0 only in static equilibrium!
Electric Field inside Metal
E
-
• No net interaction between mobile electrons
• Forget previous velocity after collision conductivity ()
μCollisions:- impurities- thermal motion of atoms
Higher temperature T shorter lower
Drude Model of Electron Motion in a Metal
∆𝑝∆ 𝑡 =𝐹 𝑛𝑒𝑡=(−𝑒)𝐸𝑛𝑒𝑡
∆ 𝑝=𝑝− 0=(−𝑒)𝐸𝑛𝑒𝑡 ∆ 𝑡
𝑣=𝑝 /𝑚𝑒=−𝑒𝐸𝑛𝑒𝑡∆ 𝑡
𝑚𝑒
𝑣=𝑒∆ 𝑡𝑚𝑒
𝐸𝑛𝑒𝑡𝜇=𝑒∆𝑡𝑚𝑒
;𝑚𝑜𝑏𝑖𝑙𝑖𝑡𝑦
Excess charges in any conductor are always found on an inner or outer surface!
Excess charges only on surface anywhere on or inside material
Distribution of excess charges Spread over entire surface located in patches
Conductors versus Insulators
Discharging by contact:
On approach: body polarizes
On contact:charge redistributes over larger surface
Grounding: connection to earth (ground) – very large object
Charging and Discharging
Charging by Induction
Charging by Induction
An object can be both charged and polarized
On a negatively charged metal ball excess charge is spread uniformly all over the surface.
What happens if a positive charge is brought near?
+
Exercise
Splitting universe into two parts does not always work.
+q
If q is so small that it does not appreciably alter the charge distribution on the sphere, then we can still use the original field:Otherwise, we must calculate new field: