electrostatics and coulombs lawsecure site gabriel/presentation 1.pdf · charge is quantized q =...
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Electromagnetism
Electromagnetism is one of the fundamental forcesin nature, and the the dominant force in a vast range
of natural and technological phenomena
The electromagnetic force is solely responsible for thestructure of matter, organic, or inorganicPhysics, chemistry, biology, materials science
The operation of most technological devices is based onelectromagnetic forces. From lights, motors, and batteries,to communication and broadcasting systems, as well asmicroelectronic devices. Engineering
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ElectromagnetismElectricity
Electromagnetism MagnetismOptics
In this course we are going to discuss the fundamental concepts of electromagnetism:
charge force field potential currentelectriccircuit
magneticfield
induction alternatingcurrents
waves
reflection refraction image interference diffraction
Once you master these basic concepts, you will be ready to move forward,into more advanced subjects in your specific field of interest
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System of UnitsWe will use the SI system – SI ≡ International System of Units
Fundamental QuantitiesLength meter [m]
Mass kilogram [kg]Time second [s]
Other UnitsCurrent ampere [A]
Derived QuantitiesForce newton 1 N = 1 kg m / s2
Energy joule 1 J = 1 N mCharge coulomb 1 C = 1 A s
Electric Potential volt 1 V = 1 J / CResistance ohm 1 Ω = 1 V / A
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Electric ChargesForces and Fields
Chapter 19
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Electric Charge
The Transfer of Charge
SILK
Glass Rod
Some materials attract electronsmore than others.
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Electric Charge
The Transfer of Charge
SILK
Glass Rod
-+
As the glass rod is rubbed against silk, electrons are pulled off the glass onto the silk.
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Electric Charge
The Transfer of Charge
SILK
Glass Rod
--+
+
Usually matter is charge neutral, because the number of electrons and protons are equal. But here the silk has anexcess of electrons and the rod a deficit.
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Electric Charge
The Transfer of Charge
SILK
Glass Rod
-
++++
+
--- -
Glass and silk are insulators:charges stuck on them stay put.
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Electric Charge
The Transfer of Charge
SILK
Glass Rod
-
++++
+
--- -
Now the glass and the silk attract each other because they have opposite charges
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Two rods with opposite charges attract each other.
Electric Charge
+ +
Two positively charged rods repel each other.
– +
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Electric Charge
History
600 BC Greeks first discover attractiveproperties of amber when rubbed.
1600 AD Electric bodies repel as well as attract1735 AD du Fay: Two distinct types of electricity1750 AD Franklin: Positive and Negative Charge1770 AD Coulomb: “Inverse Square Law”1890 AD J.J. Thompson: Quantization of
electric charge - “Electron”
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Electric Charge
Summary of things we know:
– There is a property of matter called electric charge. (In the SI system its units are Coulombs.)
– Charges can be negative (like electrons) or positive (like protons).
– In matter, the positive charges are stuck in place in the nuclei. Matter is negatively charged when extra electrons are added, and positively charged when electrons are removed.
– Like charges repel, unlike charges attract.– Charges travel in conductors, not in insulators– Force of attraction or repulsion ~ 1 / r2
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Crude representation of an atomshowing positive charges (protons)inside the nucleus, and negative charges(electrons) orbiting around the nucleus.
Conservation of Electric Charge
The total electric charge in the universe is constant
Objects get charged by exchange of charge with other objects(usually due to electron transfer from one object to another).
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Most objects contains equal amounts of positive and negativecharge, so they appear neutral on a macroscopic level
Polarization
When a charged rod is broughtclose to an object, in can distortthe internal charges, giving riseto an attractive force between rod and object.
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Uncharged amber rod exerts no force on scraps of paper (a)
When the rod is rubbed against a piece of fur, it becomes charged by charge transfer (b)
The charged rod attracts the scraps of paper by polarization (c)
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Charge is Quantized
q = multiple of an elementary charge e:e = 1.6 x 10-19 Coulombs
Charge Mass Diameterelectron - e 1 0proton +e 1836 ~10-15mneutron 0 1839 ~10-15m
positron +e 1 0
(Protons and neutrons are made up of quarks, whose charge is quantized in multiples of e/3. Quarks can’t be isolated.)
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Insulators and Conductors
In insulators, charges are not free to move long distances
In metals, charges can move macroscopic distances
Uncharged metal sphere touched by charged rod.
Initially charged is transferred at the point of contact (a)
Then, the charge spreads out (b) due to repulsion between likecharges.
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Coulomb’s Law
k = (4πε0)-1 = 9.0 x 109 Nm2/C2
ε0 = permitivity of free space = 8.86 x 10-12 C2/Nm2
Coulomb’s law describes the interaction between bodies due to their charges
1 22
q qF k
r=
The direction of the force is alongthe line connecting the charges
First calculate magnitude,then, determine direction
Notice: 12 21F F= −
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Gravitational and Electric Forces in the Hydrogen Atom
+e -eM
m
r12m = 9.1 10-31 kgM = 1.7 10-27 kgr12 = 5.3 10-11 m
Gravitational force Electric Force
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Gravitational and Electric Forcesin the Hydrogen Atom
+e -eM
m
r12m = 9.1 10-31 kgM = 1.7 10-27 kgr12 = 5.3 10-11 m
Gravitational force Electric Force
Fg = 3.6 10-47 N
F G Mmr
rg =122
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Gravitational and Electric Forces in the Hydrogen Atom
+e -eM
m
r12m = 9.1 10-31 kgM = 1.7 10-27 kgr12 = 5.3 10-11 m
Gravitational force Electric Force
Fg = 3.6 10-47 N
F G Mmr
rg =122 F Qq
rre =
⎛⎝⎜
⎞⎠⎟
14 0 12
2πε
Fe = 3.6 10-8N
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Superposition of forces from two chargesBlue charges are negative with equal charge (-q)
What is the force on the positive red charge +q ?
x
y
NETFORCE
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Superposition Principle
q3
q1
q2
F13
F12
F F13
F13x
F13y
F12y
F
F12x
12
F = (F12x + F13x) x + (F12y + F13y) y
Forces add vectorially
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Example: electricity balancing gravity
q q
m m
θl
Two identical balls, with mass m and charge q, hang from similar strings of length l.
After equilibrium is reached,find the charge q as a function of θ and l
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Example: electricity balancing gravity
q q
m m
θ lWhat forces are acting onthe charged balls ?
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• Draw vector force diagram while identifying the forces.
• Apply Newton’s 3rd
Law, for a system in equilibrium, to the components of the forces.
• Solve!
T T
FE FE
FG=mg FG=mg
Example: electricity balancing gravity