Electromagnetism Electromagnetism is one of the fundamental forces in nature, and the the dominant force in a vast range of natural and technological phenomena.

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Presentation transcript:

Electromagnetism Electromagnetism is one of the fundamental forces in nature, and the the dominant force in a vast range of natural and technological phenomena  The electromagnetic force is solely responsible for the structure of matter, organic, or inorganic  Physics, chemistry, biology, materials science   The operation of most technological devices is based on electromagnetic forces. From lights, motors, and batteries, to communication and broadcasting systems, as well as microelectronic devices.  Engineering

Electromagnetism Electricity Electromagnetism Magnetism Optics In this course we are going to discuss the fundamental concepts of electromagnetism: chargeforcefieldpotentialcurrent electric circuit magnetic field inductionalternating currents waves reflectionrefractionimageinterferencediffraction Once you master these basic concepts, you will be ready to move forward, into more advanced subjects in your specific field of interest

Electric Charge Chapter 22

Electric Charge The Transfer of Charge SILK Glass Rod Some materials attract electrons more than others.

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.

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 an excess of electrons and the rod a deficit.

Electric Charge The Transfer of Charge SILK Glass Rod Glass and silk are insulators: charges stuck on them stay put

Electric Charge ++ Two positively charged rods repel each other.

Electric Charge History 600 BCGreeks first discover attractive properties of amber when rubbed ADElectric bodies repel as well as attract 1735 ADdu Fay: Two distinct types of electricity 1750 ADFranklin: Positive and Negative Charge 1770 ADCoulomb: “Inverse Square Law” 1890 ADJ.J. Thompson: Quantization of electric charge - “Electron”

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. –Electrons travel in conductors, but not in insulators –Force of attraction or repulsion ~ 1 / r 2

System of Units We will use the SI system (Systeme Internationale) Fundamental Quantities Length  meter [m] Mass  kilogram [kg] Time  second [s] Derived Quantities Force  newton 1 N = 1 kg m / s 2 Energy  joule 1 J = 1 N m New Units Charge  coulomb 1 C = 1 A s Current  ampere [A] Electric Potential  volt 1 V = 1 J / C Resistance  ohm 1  = 1 V / A

Charge is Quantized q = multiple of an elementary charge e: e = 1.6 x Coulombs Charge MassDiameter electron - e 1 0 proton +e1836 ~ m neutron ~ m 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.)

Coulomb’s Law q1q1 q2q2 r 12 F 12 Force on 2 due to 1 k = (4  0 ) -1 = 9.0 x 10 9 Nm 2 /C 2   = permitivity of free space = 8.86 x C 2 /Nm 2 Coulomb’s law describes the interaction between bodies due to their charges

Gravitational and Electric Forces in the Hydrogen Atom +e -e M m r m = kg M = kg r = m Gravitational forceElectric Force

Gravitational and Electric Forces in the Hydrogen Atom +e -e M m r m = kg M = kg r = m Gravitational forceElectric Force F g = N

Gravitational and Electric Forces in the Hydrogen Atom +e -e M m r m = kg M = kg r = m Gravitational forceElectric Force F g = NF e = N

Superposition of forces from two charges Blue charges fixed, negative, equal charge (-q) What is force on positive red charge +q ? x y

Superposition of forces from two charges Blue charges fixed, negative, equal charge (-q) What is force on positive red charge +q ? x y Consider effect of each charge separately:

Superposition of forces from two charges Blue charges fixed, negative, equal charge (-q) What is force on positive red charge +q ? x y Take each charge in turn:

Superposition of forces from two charges Blue charges fixed, negative, equal charge (-q) What is force on positive red charge +q ? x y Create vector sum:

Superposition of forces from two charges Blue charges fixed, negative, equal charge (-q) What is force on positive red charge +q ? x y Find resultant: NET FORCE

Superposition Principle q3q3 q1q1 q2q2 F 31 F 21 F F 31 F 13 F 31x F 31y F 21x F 21y F 21 F = (F 21x + F 31x ) x + (F 21y + F 31y ) y Forces add vectorially

Simple Special Case: Spherical Charge Distributions F 13 A uniform charge sphere (or spherical shell) with total charge Q acts outside the sphere as though the charge was all concentrated at the center. But a uniform shell exerts zero force on any interior charge. Q (smeared)q1q1 q2q2

Simple Special Case: Spherical Charge Distributions F 13 A uniform charge sphere (or spherical shell) with total charge Q acts outside the sphere as though the charge was all concentrated at the center. But a uniform shell exerts zero force on any interior charge. Q (smeared)q1q1 q2q2

Simple Special Case: Spherical Charge Distributions F 13 A uniform charge sphere (or spherical shell) with total charge Q acts outside the sphere as though the charge was all concentrated at the center. But a uniform shell exerts zero force on any interior charge. Q (smeared)q1q1 q2q2

Electricity balancing gravity q q m m 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  and l  l

Example: electricity balancing gravity q q m m  l What forces are acting on the charged balls ?

Draw vector force diagram while identifying the forces. Apply Newton’s 2 nd Law, for a system in equilibrium, to the components of the forces. Solve! T T FEFE FEFE F G =mg Example: electricity balancing gravity