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The subscript r designates its time derivative in the rotating coordinate. Here's how to derive a very useful operator relation linking time derivatives in rotating and inertial frames. We'll use this relation to show how fictitious. Unit vector rotates with the rotation of the earth.
Now try to relate spherical and rectangular coordinate systems. Your group should derive expressions relating the coordinates of the two systems, expressions relating the unit. Or writing the components as column vectors etc. Now in the same way you can take another time derivative, leading to. Multiplying by the mass of the particle you get. \( {{l}}_{{g}} { \,= \,6}. Since the earth is rotating about its axis and since it is convenient to adopt a frame of reference fixed in the earth, we need to study the equations of motion in a rotating coordinate system. Observers if the unit vector rotates with the rotation of the earth. The situation is shown in figure 4. 1. 1 in a time δt the unit vector swings in under the influence of the rotation and is moved at.
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