The coordinate curves are
The straight-lines, r (θ 0 , z ), 0 ≤z≤h
and the circles, r (θ, z 0 ), 0 ≤θ≤ 2 π,
where θ 0 and z 0 are constants. The tangent vectors to the coordinate curves are
given by
∂r
∂θ =−asin θ
ˆe 1 +acos θeˆ 2 and ∂r
∂z =
ˆe 3
Consequently, we have E=a^2 , F = 0,and G= 1 .The element of surface area is then
dS =
√
EG −F^2 dθ dz =a dθ dz. The surface area of the cylinder of height his therefore
S=
∫h
0
∫ 2 π
0
a dθ dz = 2πah.
Volume Integrals
The summation of scalar and vector fields over a region of space can be expressed
by volume integrals having the form
∫∫∫
V
f(x, y, z )dV and
∫∫∫
V
F(x, y, z )dV,
where dV =dx dy dz is an element of volume and V is the region over which the
integrations are to extend.
The integral of the scalar field is an ordinary triple integral. The triple integral
of the vector function F =F(x, y, z )can be expressed as
∫∫∫
V
F dV =eˆ 1 ∫∫∫
V
F 1 (x, y, z )dV +ˆe 2
∫∫∫
V
F 2 (x, y, z )dV +ˆe 3
∫∫∫
V
F 3 (x, y, z )dV, (7 .106)
where each component is a scalar triple integral.
Whenever appropriate, the above integrals are sometimes expressed
(i) in cylindrical coordinates (r, θ, z ), where x=rcos θ, y =rsin θ, z =zand the element
of volume is represented dV =r dr dθ dz
(ii) in spherical coordinates (ρ, θ, φ )where x=ρsin θcos φ,y=ρsin θsin φ,z=ρcos θand
the element of volume is dV =ρ^2 sin θ dρ dφ dθ.
(iii) in curvilinear coordinates (u, v, w )where x=x(u, v, w ), y =y(u, v, w ), z =z(u, v, w )
and the element of volume is given by^8 dV =
∣∣
∣∣∂r
∂u ·
(
∂r
∂v ×
∂r
∂w
)∣∣
∣∣du dv dw where
r =x(u, v, w )ˆe 1 +y(u, v, w )ˆe 2 +z(u, v, w )ˆe 3
(^8) See pages 143 and 156 for details.