It can be proved that if a bounded plane region slides along a helix in such a way that the region is always orthogonal to the helix (i.e., orthogonal to the unit tangent vector to the helix), then the volume swept out by the region is equal to the area of the region times the distance traveled by its centroid. Use this result to find the volume of the “tubeâ€� in the accompanying figure that is swept out by sliding a circle of radius 1 2 along the helix x = cos t , y = sin t , z = t 4 0 ≤ t ≤ 4 π in such a way that the circle is always centered on the helix and lies in the plane perpendicular to the helix.
It can be proved that if a bounded plane region slides along a helix in such a way that the region is always orthogonal to the helix (i.e., orthogonal to the unit tangent vector to the helix), then the volume swept out by the region is equal to the area of the region times the distance traveled by its centroid. Use this result to find the volume of the “tubeâ€� in the accompanying figure that is swept out by sliding a circle of radius 1 2 along the helix x = cos t , y = sin t , z = t 4 0 ≤ t ≤ 4 π in such a way that the circle is always centered on the helix and lies in the plane perpendicular to the helix.
It can be proved that if a bounded plane region slides along a helix in such a way that the region is always orthogonal to the helix (i.e., orthogonal to the unit tangent vector to the helix), then the volume swept out by the region is equal to the area of the region times the distance traveled by its centroid. Use this result to find the volume of the “tube� in the accompanying figure that is swept out by sliding a circle of radius
1
2
along the helix
x
=
cos
t
,
y
=
sin
t
,
z
=
t
4
0
≤
t
≤
4
π
in such a way that the circle is always centered on the helix and lies in the plane perpendicular to the helix.
Quantities that have magnitude and direction but not position. Some examples of vectors are velocity, displacement, acceleration, and force. They are sometimes called Euclidean or spatial vectors.
Show that the Laplace equation in Cartesian coordinates:
J²u
J²u
+
= 0
მx2 Jy2
can be reduced to the following form in cylindrical polar coordinates:
湯(
ди
1 8²u
+
Or 7,2 მ)2
= 0.
Find integrating factor
Draw the vertical and horizontal asymptotes. Then plot the intercepts (if any), and plot at least one point on each side of each vertical asymptote.
Chapter 14 Solutions
Calculus Early Transcendentals, Binder Ready Version
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Area Between The Curve Problem No 1 - Applications Of Definite Integration - Diploma Maths II; Author: Ekeeda;https://www.youtube.com/watch?v=q3ZU0GnGaxA;License: Standard YouTube License, CC-BY