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or a frame F1​, we do the following transformations. a) rotate F1​ by a rotation matrix R21​ with respect to F1​ to get frame F2​. b) translate F2​ by a displacement vector d12​ to get frame F3​. c) rotate F3​ by a rotation matrix R32​ with respect to F3​ to get frame F4​."

User Dechen
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Final answer:

The student's question involves physics concepts involving reference frame transformations, rotational kinematics, and mechanics at the college level. It specifically addresses how coordinates change through rotations and translations, and how these relate to forces and motion of rigid bodies.

Step-by-step explanation:

The question relates to the transformations of reference frames in physics, specifically in the context of rotational kinematics and mechanics.

When a frame F1 undergoes a rotation represented by a rotation matrix R21, followed by a translation by a vector d12, and another rotation represented by R32, it is transformed sequentially into frames F2, F3 and finally F4.

These transformations are mathematical operations that describe how the position and orientation of the frame are altered in space.

In the process of these transformations, we use mathematical expressions to relate coordinates in the new and old reference frames.

For instance, during a rotation transformation, the coordinates in the new frame (S') are related to coordinates in the original frame (S) by the following equations: x' = x cos q + y sin q and y' = -x sin q + y cos q.

These equations are derived considering a rigid body rotating around a fixed axis without any translation—represented by an object like a flywheel fixed in space.

User Mars Redwyne
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a) Rotate F1 by a rotation matrix R21 with respect to F1 to get frame F2.

b) Translate F2 by a displacement vector d12 to get frame F3.

c) Rotate F3 by a rotation matrix R32 with respect to F3 to get frame F4.
User Vyacheslav Volkov
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