Class Notes for Electrical and Computer Engineering at University of Waterloo
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ECE106 Lecture 71: ECE 106,University of Waterloo,(p71)
Example 3 An infinite wire has been bend. Calculate B at point P....
ECE106 Lecture 72: ECE 106,University of Waterloo,(p72)
So for semiinfinite wire AO, 0 0 dl r dB = 4 r2 is nothing but equa...
ECE106 Lecture 73: ECE 106,University of Waterloo,(p73)
From example 1, 0J 0 B = r 1 1 1 0 0 B = r 2 2 2 2 B = B +1B 2 0 0 ...
ECE106 Lecture 74: ECE 106,University of Waterloo,(p74)
Because z = y. Therefore B is: 190
ECE106 Lecture 67: ECE 106,University of Waterloo,(p67)
Example 1 Magnetic field of a cylindrical conductor. An infinite lo...
ECE106 Lecture 69: ECE 106,University of Waterloo,(p69)
Let us consider the line AA, dB due to element on left and right ar...
ECE106 Lecture 70: ECE 106,University of Waterloo,(p70)
So, consider this: By Amperes Law: I B dl = I0 enc Bl f r oAB + 0 f...
ECE106 Lecture 66: ECE 106,University of Waterloo,(p66)
1. For z =0. 0 2 3 0 ...
ECE106 Lecture 63: ECE 106,University of Waterloo,(p63)
dU By definition, power is consumed (or flow) per unit time, i.e. P...
ECE106 Lecture 68: ECE 106,University of Waterloo,(p68)
For r a B 2r = I 0enc =...
ECE106 Lecture 61: ECE 106,University of Waterloo,(p61)
In a perfect conductor (metal) there is only one type of carrier fr...
ECE106 Lecture 64: ECE 106,University of Waterloo,(p64)
idl dl R l P Bisecting line Figure 8.2: Example 1. Note: This direc...
ECE106 Lecture 58: ECE 106,University of Waterloo,(p58)
For R < R i I ...
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