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Learn about magnetic fields, forces on conductors, DC motors, right-hand rule, Ampere's Law, magnetic energy density, and inductance calculations in EEE-161 Electromagnetics - Magnetostatics with Dr. Markovic.
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Magnetostatics EEE 161 EEE 161 Electromagnetics - Magnetostatics Dr. Markovic
Learning Objectives • Students will be able to • Apply cross product (right-hand rule) • Visualize magnetic field from a straight conductor • Calculate the magnetic force • On a conductor in an external magnetic field • Between two current-carrying conductors • Explain operation of a simple DC-motor EEE 161 Electromagnetics - Magnetostatics Dr. Markovic
Force on a conductor EEE 161 Electromagnetics - Magnetostatics Dr. Markovic
Force on a conductor EEE 161 Electromagnetics - Magnetostatics Dr. Markovic
Force on a conductor EEE 161 Electromagnetics - Magnetostatics Dr. Markovic
Magnetic Force on a Current Element If the field was coming out of the page EEE 161 Electromagnetics - Magnetostatics Dr. Markovic
Right Hand Rule Number of magnetic field lines unit is Weber http://en.wikipedia.org/wiki/File:Manoderecha.svg EEE 161 Electromagnetics - Magnetostatics Dr. Markovic
Force between two conductors EEE 161 Electromagnetics - Magnetostatics Dr. Markovic
Force between two conductors EEE 161 Electromagnetics - Magnetostatics Dr. Markovic
Force between two conductors EEE 161 Electromagnetics - Magnetostatics Dr. Markovic
Magnetic Force on a Current Element EEE 161 Electromagnetics - Magnetostatics Dr. Markovic
Socrative Quiz #1 EEE 161 Electromagnetics - Magnetostatics Dr. Markovic
Magnetic Force on a Current Loop EEE 161 Electromagnetics - Magnetostatics Dr. Markovic
Socrative Quiz #2 EEE 161 Electromagnetics - Magnetostatics Dr. Markovic
MS#1 Loop of current is given. It is fixed in the middle of top and bottom wires. Magnetic flux density B. Find the direction of the forces on the loop and CW, CCW? EEE 161 Electromagnetics - Magnetostatics Dr. Markovic
How do we find H? Ampere’s law Bio-Savart’s Law How do we find E? Gauss’ Law Coulomb’s Law EEE 161 Electromagnetics - Magnetostatics Dr. Markovic
Ampère’s Law EEE 161 Electromagnetics - Magnetostatics Dr. Markovic
Guided Example: Magnetic field of an infinite line of current 1. What is the direction of magnetic field? 2.Then we have to pick an appropriate contour (we pick circle because the magnetic field is constant on this circle – all points are the same distance away from the wire) 3. What is the contour piece dl? EEE 161 Electromagnetics - Magnetostatics Dr. Markovic
What is the direction of magnetic field? Magnetic field on this circle will be constant (all points are the same distance away from the source (current) EEE 161 Electromagnetics - Magnetostatics Dr. Markovic
Why can we take H in front of the integral? Why is H a constant? EEE 161 Electromagnetics - Magnetostatics Dr. Markovic
Radius of wire a EEE 161 Electromagnetics - Magnetostatics Dr. Markovic
Example: Internal Magnetic Field of Long Conductor For r < a EEE 161 Electromagnetics - Magnetostatics Dr. Markovic Cont.
MS#2 Find the magnetic field everywhere around an infinite hollow cylindrical conductor shown. J=const (current density). Given: I, a, b. Find H. EEE 161 Electromagnetics - Magnetostatics Dr. Markovic
How is B different than H? H – magnetic field B- magnetic flux density Magnetic permeability How is D different than E? E – electric field D- electric flux density electric permittivity EEE 161 Electromagnetics - Magnetostatics Dr. Markovic
How can you calculate inductance? EEE 161 Electromagnetics - Magnetostatics Dr. Markovic
How can you calculate inductance? Magnetostatic energy Electrostatic energy EEE 161 Electromagnetics - Magnetostatics Dr. Markovic
Example: Using Magnetic Energy Density to find Inductance Magnetic field in the insulating material is Current is given EEE 161 Electromagnetics - Magnetostatics Dr. Markovic
Example:Magnetic Energy Density Magnetic field in the insulating material is The magnetic energy stored in the coaxial cable is EEE 161 Electromagnetics - Magnetostatics Dr. Markovic
Example:Magnetic Energy Density The magnetic energy stored in the coaxial cable is EEE 161 Electromagnetics - Magnetostatics Dr. Markovic
Graded Quiz MS#3 • Using magnetic energy density equation, find the internal inductance of a wire of circular cross section, with radius of a=1mm. The current is constant throughout the wire. EEE 161 Electromagnetics - Magnetostatics Dr. Markovic
Inductance recall • Inductor creates magnetic field • Current in one conductor will cause current in another conductor that’s mutual inductance • J omega L • Inductor resists current changes • Voltage over inductor is inductance x di/dt • Positive VAR EEE 161 Electromagnetics - Magnetostatics Dr. Markovic
Conceptual understanding of inductance EEE 161 Electromagnetics - Magnetostatics Dr. Markovic
There are circular rings of magnetic-field around all currents EEE 161 Electromagnetics - Magnetostatics Dr. Markovic
Right Hand Rule Number of magnetic field lines unit is Weber http://en.wikipedia.org/wiki/File:Manoderecha.svg EEE 161 Electromagnetics - Magnetostatics Dr. Markovic
Learning Outcomes • Students will be able to • Describe inductance through flux of magnetic field • Conceptually explain what is inductance • Describe what affects inductance • Estimate inductance EEE 161 Electromagnetics - Magnetostatics Dr. Markovic
Resistance • Resistance is defined as • Do we have any such equations for inductance and capacitance? EEE 161 Electromagnetics - Magnetostatics Dr. Markovic
Capacitance and Inductance do not relate directly current and voltage. EEE 161 Electromagnetics - Magnetostatics Dr. Markovic