Understanding Vector Magnitude and Direction in Mechanics

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The discussion centers on a question regarding the derivation of the equation |\triangle A|=2Asin(\frac{\triangle\theta}{2}) from Klppner's "An Introduction to Mechanics." The angle \Delta\theta is identified as the angle between the vectors A(t) and A(t+\Delta t), which are of constant magnitude A. The derivation involves using the law of cosines and trigonometric identities to relate the change in vector magnitude to the angle between the vectors. The equation becomes more precise as \Delta\theta decreases, and the geometry of the situation is explained through the construction of an isosceles triangle formed by the vectors. The conversation also includes a light-hearted exchange about the cost of the book.
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my question is from klppner's text an introduction to mechanics, on page 26, they suppose a vector A(t) has a constant magnitude A, he states that the direction dA(t)/dt is always perpendicular to A(t), now they define \triangle A=A(t+\triangle t)-A(t), he states that |\triangle A|=2Asin(\frac{\triangle\theta}{2}) i don't understand how did they arrive at the last equation, and don't understand which angle does he refer to. he states that it's defined in a sketch in the book but i can't find where does he state this?

thanks in advance.
 
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I don't have the book with me now, but I think \Delta\theta is the angle between the A(t) and A(t+\Delta t). The equation becomes more accurate as the angle becomes smaller.
 
\Delta \theta is the angle betweenA(t+\triangle t) and A(t). Since both vectors are of magnitude A, the law of cosines gives

\Delta A^2 = A^2+A^2-2AAcos(\Delta \theta)

And cos(2x) = 1 - 2sin^2(x), so...
 
Ok, Draw a vector for A(t), and then draw another for A(t+\triangle t) with the same length and starting from the same point in space. The angle \triangle\theta is acute angle between these two vectors and \triangle A is the vector that forms the third side of the isosceles triangle having A(t) and A(t+\triangle t) for sides (and it terminates in the same place A(t+\triangle t) does). Construct the altitude of this triangle and consider one of the resulting identical right triangles with one leg being the altitude, one leg is of length \frac{1}{2}\left| \triangle A\right|, and the hypotenuse is of length A. Use trig.
 
|\Delta A| = \sqrt{(A(t+\Delta t)-A(t))\cdot(A(t+\Delta t)-A(t))}

= \sqrt{|A(t+\Delta t)|^2 - 2A(t+\Delta t)\cdot A(t) + |A(t)|^2}<br /> = \sqrt{A^2 - 2A^2\cos {\Delta \theta} + A^2}

= \sqrt{2A^2 - 2A^2\cos{\Delta \theta}} = \sqrt{2}A\sqrt{1-\cos{\Delta \theta}}.

Now use the identity \sin^2{\phi} = \frac{1}{2}(1-\cos{2\phi}) to change that into

\sqrt{2}A\sqrt{2\sin^2{\frac{\Delta \theta}{2}}}

= 2A\sin \frac{\Delta \theta}{2}.

Here, \Delta \theta is the angle between A(t+\Delta t) and A(t) and A is the (constant) magnitude of the vector function.
 
thank you for your help.
 
by the way, neutrino, you haven't bought the booog, have you?
ive seen in amazon that it's quite coasts a lot.
 
loop quantum gravity said:
by the way, neutrino, you haven't bought the booog, have you?
ive seen in amazon that it's quite coasts a lot.
What's that? Some new variant for the word book?
 
no just big funny typing error.
 
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