Tick the correct boxes. i. In variable changes of plane and space integrals, the local magnification ratio of the area or volume is always the same as the Jacobian determinant of the transformation. ii. In the variable change of the plane integral, the magnification ratio of the area is constant (i.e. does not depend on the examined point), if the variable change is linear, i.e. x=au+bv, y=cu+dv, when a,b,c,d∈R are constant. iii. In the spherical coordinate system, dV=r2sinφdrdφdθ . iv. In the spherical coordinate system, dV=drdS , when dS is interpreted as a surface element on the surface of a sphere of radius r. v. In the cylindrical coordinate system, dV=r⊥dr⊥dθdz
Tick the correct boxes. i. In variable changes of plane and space integrals, the local magnification ratio of the area or volume is always the same as the Jacobian determinant of the transformation. ii. In the variable change of the plane integral, the magnification ratio of the area is constant (i.e. does not depend on the examined point), if the variable change is linear, i.e. x=au+bv, y=cu+dv, when a,b,c,d∈R are constant. iii. In the spherical coordinate system, dV=r2sinφdrdφdθ . iv. In the spherical coordinate system, dV=drdS , when dS is interpreted as a surface element on the surface of a sphere of radius r. v. In the cylindrical coordinate system, dV=r⊥dr⊥dθdz
Advanced Engineering Mathematics
10th Edition
ISBN:9780470458365
Author:Erwin Kreyszig
Publisher:Erwin Kreyszig
Chapter2: Second-order Linear Odes
Section: Chapter Questions
Problem 1RQ
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Question
Tick the correct boxes.
i. In variable changes of plane and space
ii.
In the variable change of the plane integral, the magnification ratio of the area is constant (i.e. does not depend on the examined point), if the variable change is linear, i.e. x=au+bv, y=cu+dv, when a,b,c,d∈R are constant.
iii.
In the spherical
.
iv.
In the spherical coordinate system, dV=drdS
, when dS is interpreted as a surface element on the surface of a sphere of radius r.
v.
In the cylindrical coordinate system, dV=r⊥dr⊥dθdz
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