Time derivative of rotating vector

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SUMMARY

The discussion centers on understanding the time derivative of a rotating vector, specifically the relationship between the change in vector magnitude, ΔA, and the angle of rotation, θ. The key equation derived is |ΔA| = 2A sin(Δθ/2), which is established through geometric reasoning and the application of the half-angle trigonometric identity. The derivation involves calculating ΔA as the difference between the vector positions before and after rotation, ultimately leading to the conclusion that visualizing the problem geometrically aids in comprehending the relationship between the angle and the vector change.

PREREQUISITES
  • Understanding of basic vector mathematics
  • Familiarity with trigonometric identities, particularly the half-angle identity
  • Knowledge of rotational motion concepts in physics
  • Ability to apply the Pythagorean theorem in geometric contexts
NEXT STEPS
  • Study the derivation of vector rotation in physics using Kleppner's "An Introduction to Mechanics"
  • Learn about the applications of trigonometric identities in physics problems
  • Explore the concept of angular velocity and its relation to vector derivatives
  • Practice visualizing vector changes through geometric sketches and diagrams
USEFUL FOR

Students of physics, particularly those studying mechanics, educators teaching vector mathematics, and anyone interested in the geometric interpretation of rotational motion.

Wardub
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Trying to teach myself physics and I've run into a problem I don't quite understand.

"The magnitude of dA/dt can be found by the following geometrical argument. The change of A in the time interval t to Δt is"

ΔA = A(t + Δt) - A(t)

And then somehow it gets to
A| = 2Asin(Δ[itex]\theta[/itex]/2)

I just can't see how those are equal. Especially where theta/2 comes in.
This comes out of Kleppner pages 25 and 26, if that helps. Supposedly there's a sketch, but I can't see one.
 
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Work it out. Suppose at t = 0, A points along the x-axis, so A = (A,0), If you rotate by an amount theta, the A = (A cos(theta),A sin(theta). So Delta A = (A(1-cos(theta)),A sin(theta)). So:

[tex]|\Delta A| =A \sqrt{(1-\cos(\theta)^2 + \sin(\theta)^2} =A \sqrt{1-2\cos(\theta) + \cos(\theta)^2 + \sin(\theta)^2} =A \sqrt{2-2\cos(\theta)} = 2A \sin(\frac{\theta}{2})[/tex]

This last is a half-angle trig identity:

[tex]\sin(\frac{\theta}{2}) = \sqrt{\frac{1-\cos(\theta)}{2}}[/tex]
 
Thanks, I actually just got it myself by drawing a picture and using the Pythagorean theorem. Essentially equivalent to what you did.
 

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