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mathematical_physics_2007_21.pdf
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x = pcos
y = psin+ (3.5)
and the corresponding inverse equations
p = d w
4 = tan-' ( Y h ) (3.6)
govern the relationship between cylindrrcal coordinates and the coordinates of a
The unit basis vectors for the cylindrical system are shown in Figure 3.2(b). Each basis vector points in the direction that P moves when the corresponding coordinate is increased. For example, the direction of SP is found by watching how P moves as p is increased. This method can be used to determine the directions of basis vectors
undefined. The cylindrical coordinates, taken in the order ( p , 4, z ) , form a right-handed sys- tem. If you align your right hand along GP, and then curl your fingers to point in the
orthononnal since
6 ,. 6 , = 6,. Q = Q. e+ = 0
e,. _ p_* = e,. c, = c,. Q = 1.
The position vector expressed in cylindrical coordinates is
r"
X
z 6,
X
Figure 3.2 The Cylindrical System
THE CYLINDRICAL SYSTEM 47
Y r
$ e @ 6 P
X eP Figure 3.3 The Position Vector in a Cylindrical System
Notice that C+ is always perpendicular to F, as shown in Figure 3.3, so Equation 3. reduces to
dinates, is called a polar system. This system, shown in Figure 3.4(a), has basis vectors C, and C+. The position vector, shown in Figure 3.4(b), has only a p-component and is expressed as
Remember an arbitrary vector v, unlike the position vector, can have both p- and 4-
(b) Figure 3.4 The Polar System
Figure
v@ dVe P
VP P (^) X ~~ 3.5 (^) Polar Components of a Vector