Electricity and Magnetism - MIT OpenCourseWare · Electricity and Magnetism •Today – Electric...
Transcript of Electricity and Magnetism - MIT OpenCourseWare · Electricity and Magnetism •Today – Electric...
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Feb 25 2002
Electricity and Magnetism
• Today– Electric Potential Energy– Electric Potential– Example of calculation– Practical applications– Conductors, Isolators and Semi-Conductors
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Feb 25 2002
Recap
• Work in the Electrostatic Field• Electrostatic Potential Energy• Electrostatic Potential
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Feb 25 2002
Work and Electrostatic Force
+Q
b
a+q
Charge q at point a in Coulomb field of Q
How much work to move to point b?
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Feb 25 2002
+Q
a
dl
r+q α
b
FES is conservative!
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Feb 25 2002
Electric Potential Energy
• Note: What we used was the fact that Coulomb Force is radial (i.e. F || r)– all radial forces are conservative (e.g.
Gravity)
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Feb 25 2002
Electric Potential Energy• Potential Energy for two charges
• Can only observe differences in potential– often set U( ) = 0 or U(earth) = 0– U(r) energy needed to bring q,Q together
from infinity
8
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Feb 25 2002
Electric Potential
• Electric Potential Energy proportional to q• Define V = U/q
• Electric Potential V: – Units are Volt [V] = [J/C]
V = U/q
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Feb 25 2002
Electric Potential
• Note: because V = U/q -> U = V q– for a given V, U can be positive or negative,
depending on sign of q
• Example: Single Charge
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Feb 25 2002
Electric Potential for many charges
• Superposition principle....
• Sum of scalars, not vectors!• Integral for continous distributions
V(r) = Σ1/(4πε0) Qi/ri
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Feb 25 2002
Electric Potential for many charges
• Electric potential depends on charges that create field, not the test charge!
• V tells us how much energy a charged object can aquire when moving from a to b
V(r) = Σ1/(4πε0) Qi/ri
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Feb 25 2002
Electrical potentials
• Battery: 1.5 V• Power outlet: 120 V• HV power line: 106 V• Accelerators: 108 V• Thunderstorm: 108 V
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Feb 25 2002
Example: Capacitor plates
• Deposite opposite charges on plates
• What is the Electric Potential?– What does E look like?
• Move charge +q from a to b
+++++++++++
-----------
ba+q
xa xbxa xb
x=0x
x=d
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Feb 25 2002
Example: Capacitor plates
+++++++++++
-----------
ba+q
xa xb
x=0x
x=d
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Feb 25 2002
Example: Capacitor plates
+++++++++++
-----------
ba+q
xa xb
x
V(x)
xx=0
x
U(x,q)
0
q>0
q<0
x=d
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Feb 25 2002
Demo: Ping-Pong Ball
+++--
-
-----------
+++++++++++
q>0
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Feb 25 2002
Demo: Ping-Pong Ball
+++++++++++
-----------
q>0
+++++
x
V(x)0
x
x
U(x,q)
q>0
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Feb 25 2002
Demo: Ping-Pong Ball
+++++++++++
-----------
q<0
x
V(x)0
x
x
U(x,q)
- -- -
-
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Feb 25 2002
Demo: Ping-Pong Ball
• Field not perfectly uniform:– Net Force on Dipole
+++++++++++
-----------
+++--
-
x
V(x)0
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Feb 25 2002
Trick question: Why does it start?
x
V(x)0+
++++++++++
-----------
+++--
-
Slope dV/dx~ E ~ F !
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Feb 25 2002
Applications
+++++++++++
-----------
+qVelocity v
d
• Energy for single particle (e.g. electron) small
• Often measured in ‘Electron Volt’ [eV]
• Energy aquired by particle of charge 10-19 C going through ∆V=1V
• Independent of d
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Feb 25 2002
ApplicationsRelativistic Heavy Ion Collider
Cathode Ray TubeRHIC
∆V
Ekin ~ 10 keV (104eV) Ekin ~ 100 GeV (1011eV)
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Feb 25 2002
Conductors
• Important for next few weeks– Electrical Circuits
• Why are some materials conductive?– All materials contain electrical charges!
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Feb 25 2002
ConductivityMicroscopic view
Metal: e- can move around freelyU(x)
e-
x
x
Insulator: e- stuck in placeU(x)
e-
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Feb 25 2002
Conductivity
x
U(x)
e-
• How can we get charges ‘unstuck’?– Give them enough energy to jump out of
potential wells
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Feb 25 2002
In-Class Demo
Charged Ions
+++
+++
++++++
+
Electroscope
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Feb 25 2002
In-Class DemoIons discharge Electroscope Charged Ions
++
++
++
++
Electroscope
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Feb 25 2002
Important application
x
U(x)
∆U ~ 0.5 eV
• Semi-conductor– # of charges controllable (by T and V)– At T=0oC Ekin ~ 1/40 eV– Basis of all Electronic Circuits (e.g. Computers)
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Feb 25 2002
Conductivity
• Note: Usually, charge carried by electrons, but not always– ‘holes’ (i.e. missing electrons) in semi-
conductors
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Feb 25 2002
Conductors
• E = 0 inside – otherwise charges would move
• No charges inside – Gauss
• E perpendicular to surface– otherwise charges on surface would move
• Potential is constant on conductor
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Feb 25 2002
Conductors
• Potential is constant on conductor