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--- 184_notes:q_path [2019/01/04 03:17] – dmcpadden
+++ 184_notes:q_path [2021/06/10 01:13] – bartonmo
@@ Line 1: / Line 1: @@
 Section 20.1 in Matter and Interactions (4th edition)
-[[184_notes:superposition_b|Next Page: Superposition]]
+/*[[184_notes:superposition_b|Next Page: Superposition]]
-[[184_notes:q_b_force|Previous Page: Magnetic Force on Moving Charges]]
+[[184_notes:q_b_force|Previous Page: Magnetic Force on Moving Charges]]*/
 ===== Path of a Charge through a Magnetic Field =====
@@ Line 9: / Line 9: @@
 {{youtube>IXc5feWSxsE?large}}
-==== Path of the Moving Charge ====
+===== Path of the Moving Charge =====
 [{{  184_notes:week11_3.png?150|Force felt by a charge moving through a B field in the -x direction}}]
@@ Line 22: / Line 22: @@
-==== Work Done ====
+===== Work Done =====
 [{{  184_notes:week11_5.png?400|Trajectory of a particle moving through a constant magnetic field at a constant speed}}]
@@ Line 35: / Line 35: @@
 This also means that we do not have a way to define a magnetic potential or a magnetic potential energy in the same way that we did with electric fields. It turns out that we can define a [[https://en.wikipedia.org/wiki/Vector_potential|vector potential]], which you may talk about in your future courses.
-==== Examples ====
+===== Examples =====
 [[:184_notes:examples:Week10_radius_motion_B_field|Radius of Circular Motion in a Magnetic Field]]
 [[:184_notes:examples:Week10_helix|Helical Motion in a Magnetic Field]]