Magnetic Effect of Current

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1 P15-Class 15: OutlineHour 1:Magnetic ForceExpt. 6: Magnetic ForceHour 2:Creating B Fields: Biot-Savart2 P15-Last Time:Magnetic Fields& Magnetic Dipoles3 P15-Magnetic FieldsBq=×FvB􀁇􀁇􀁇Magnetic Dipoles Create and Feel B Fields:Also saw thatmoving charges feel a force:4 P15-What Kind of Motion Does this Lead to?5 P15-Cyclotron Motion(1) r : radius of the circle 2mvqvBr=mvrqB⇒=(2) T : period of the motion 22rmTvqBππ==2vqBfrmωπ===(3) ω : cyclotron frequency6 P15-Current Carrying Wires7 P15-Bq=×FvB􀁇􀁇􀁇Magnetic Force on Current-Carrying Wire()mcharges=×B􀁇()BI=×FLB􀁇􀁇􀁇chargems=×B􀁇8 P15-Demonstration:Jumping Wire9 P15-Magnetic Force on Current-Carrying WireCurrent is moving charges, and we know that moving charges feela force in a magnetic field10 P15-PRS Questions:5 Predictions For Experiment 611 P15-Experiment 6:Magnetic Force 12 P15-Mid-term Course Evaluation13 P15-Lab Summary:Currents FEEL Forces in Magnetic FieldsQuestion:What happens if currents are next to each other?14 P15-Demonstration:Parallel & Anti-Parallel Currents15 P15-How Do They Interact?Moving charges also createmagnetic fields!The current in one wire createsa magnetic field that is feltby the other wire. This is the rest of today’s focus(http://ocw.mit.edu/ans7870/8/8.02T/f04/vis(http://ocw.mit.edu/ans7870/8/8.02T/f04ualizations/magnetostatics/13-/visualizations/magnetostatics/14-ParallelWires/13-SeriesWires/14-Series_320.htmlParallel_Wires_320_f185.html))16 P15-Sources of Magnetic Fields:Biot-Savart17 P15-Electric Field Of Point ChargeAn electric charge produces an electric field: rˆ21ˆ4oqrπε=Er􀁇rˆ: unit vector directed from q to P18 P15-Magnetic Field Of Moving ChargeMoving charge with velocity v produces magnetic field:2ˆx4oqrµπ=vrB􀁇􀁇:ˆrrˆPunit vector directed from q to Ppermeability of free space70410Tm/Aµπ−=×⋅19 P15-The Biot-Savart LawCurrent element of length dscarrying current I produces a magnetic field:20ˆ4rdIrsBd×=􀁇􀁇πµ(http://ocw.mit.edu/ans7870/8/8.02T/f04/visualizations/magnetostatics/03-CurrentElement3d/03-cElement320.html)20 P15-The Right-Hand Rule #2ˆˆˆ×=zρφ21 P15-Animation: Field Generated by a Moving Charge (http://ocw.mit.edu/ans7870/8/8.02T/f04/visualizations/magnetostatics/01-MovingChargePosMag/01-MovChrgMagPos_f223_320.html)22 P15-Demonstration:Field Generated by Wire23 P15-Example : Coil of Radius RConsider a coil with radius Rand current IIIIPFind the magnetic field B at the center (P)24 P15-Example : Coil of Radius RConsider a coil with radius Rand current IIIIP1) Think about it:•Legs contribute nothingIparallel to r•Ring makes field into page2) Choose a ds3) Pick your coordinates4) Write Biot-Savart25 P15-Example : Coil of Radius RIn the circular part of the coil…ˆd⊥sr􀁇ˆ|d|ds→×=sr􀁇rˆs􀁇dIII02ˆ4dIdBrµπ×=sr􀁇Biot-Savart:024Idsrµπ=024IRdRµθπ=04IdRµθπ=26 P15-Example : Coil of Radius RConsider a coil with radius Rand current I04IddBRµθπ=2004IdBdBRπµθπ==∫∫()2000244IIdRRπµµθπππ==∫IIIθs􀁇d0into page2IRµ=B􀁇27 P15-Example : Coil of Radius RNotes:•This is an EASY Biot-Savart problem:•No vectors involved•This is what I would expect on examIIPIpage into20RIµ=B􀁇28 P15-PRS Questions:B fields Generated by Currents29 P15-Group Problem:B Field from Coil of Radius RConsider a coil with radius Rand carrying a current IWARNING:This is much harder than what I just did! Why??What is B at point P?30 P15-Field Pressures and Tensions:A Way To Understand the qVxBMagnetic Force31 P15-Tension and Pressures Transmitted by E and BFields(E or B):•Transmit tension along field direction (Field lines want to pull straight)•Exert pressure perpendicular to field (Field lines repel)32 P15-Example of E Pressure/Tension(http://ocw.mit.edu/ans7870/8/8.02T/f04/visualizations/electrostatics/11-forceq/11-ForceQ_f0_320.html)Positive charge in uniform (downward) E fieldElectric force on the charge is combination of 1.Pressure pushing down from top 2.Tension pulling down towards bottom33 P15-Example of B Pressure/TensionPositive charge moving out of page in uniform (downwards) B field. Magnetic force combines:1.Pressure pushing from left 2.Tension pulling to right(http://ocw.mit.edu/ans7870/8/8.02T/f04/visualizations/magnetostatics/10-forcemovingq/10-ForceMovingQ_f0_320.html)

Description
Motion of charged particles in a magnetic field is briefly reviewed.Three dimensional illustrations showing force experienced by a current carrying conductor show how the magnetic fields interact. The steps for calculating magnetic field due to a coil is explained in detail which is usually not found in regular textbooks. And lastly it discusses the tension and pressure transmitted by electric and magnetic field.


Physics Department Faculty, Lecturers, and Technical Staff, 8.02 Physics II: Electricity and Magnetism, Massachusetts Institute of Technology: MIT OpenCourseWare),http://ocw.mit.edu (Accessed Aug 27th,2011). License: Creative Commons BY-NC-SA: http://ocw.mit.edu/terms/#cc

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