2. Derive the component transformation equations for tensors shown be- low where [C] = [BA] is the direction cosine matrix from frame A to B. B[T] = [C]^[T][C]T 3. The transport theorem for vectors shows that the time derivative can be constructed from two parts: the first is an explicit frame-dependent change of the vector whereas the second is an active rotational change of the vector. The same holds true for tensors. Starting from the previous result, derive a version of transport theorem for tensors. [C] (^[T])[C] = dt d B dt B [T] + [WB/A]B[T] – TWB/A] (10 pt) (7pt)
2. Derive the component transformation equations for tensors shown be- low where [C] = [BA] is the direction cosine matrix from frame A to B. B[T] = [C]^[T][C]T 3. The transport theorem for vectors shows that the time derivative can be constructed from two parts: the first is an explicit frame-dependent change of the vector whereas the second is an active rotational change of the vector. The same holds true for tensors. Starting from the previous result, derive a version of transport theorem for tensors. [C] (^[T])[C] = dt d B dt B [T] + [WB/A]B[T] – TWB/A] (10 pt) (7pt)
Elementary Linear Algebra (MindTap Course List)
8th Edition
ISBN:9781305658004
Author:Ron Larson
Publisher:Ron Larson
Chapter4: Vector Spaces
Section4.5: Basis And Dimension
Problem 69E: Find a basis for R2 that includes the vector (2,2).
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Question
![2. Derive the component transformation equations for tensors shown be-
low where [C] = [BA] is the direction cosine matrix from frame A to
B.
B[T] = [C]^[T][C]T
3. The transport theorem for vectors shows that the time derivative can
be constructed from two parts: the first is an explicit frame-dependent
change of the vector whereas the second is an active rotational change
of the vector. The same holds true for tensors. Starting from the
previous result, derive a version of transport theorem for tensors.
[C] (^[T])[C] =
dt
d
B
dt
B
[T] + [WB/A]B[T] – TWB/A]
(10 pt)
(7pt)](/v2/_next/image?url=https%3A%2F%2Fcontent.bartleby.com%2Fqna-images%2Fquestion%2Fea66a8de-61b8-4a80-955c-574c3532b05e%2F6ed62634-5706-4eaf-b945-078464c34ed1%2Fmnz3zgk_processed.png&w=3840&q=75)
Transcribed Image Text:2. Derive the component transformation equations for tensors shown be-
low where [C] = [BA] is the direction cosine matrix from frame A to
B.
B[T] = [C]^[T][C]T
3. The transport theorem for vectors shows that the time derivative can
be constructed from two parts: the first is an explicit frame-dependent
change of the vector whereas the second is an active rotational change
of the vector. The same holds true for tensors. Starting from the
previous result, derive a version of transport theorem for tensors.
[C] (^[T])[C] =
dt
d
B
dt
B
[T] + [WB/A]B[T] – TWB/A]
(10 pt)
(7pt)
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