Verify Book Solution for Radius of Curvature Problem

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SUMMARY

The discussion centers on verifying the speed of a projectile at a specific radius of curvature. A projectile launched at an angle of 25 degrees with an initial velocity of 60 ft/s was analyzed, revealing that the speed at which the radius of curvature is 3/4 of its initial value is indeed 54.5 ft/s, as stated in the book solution. The radius of curvature formula used is R = |v|³ / |v × ẋ|, confirming that the speed is proportional to the cube root of the curvature ratio. The calculations demonstrate that the book's solution is accurate and consistent with the physics of projectile motion.

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  • Knowledge of vector calculus, specifically cross products
  • Basic physics concepts including acceleration due to gravity (g)
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  • Study the derivation of the radius of curvature in projectile motion
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  • Investigate the implications of varying launch angles on projectile speed and curvature
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skeeter
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I was helping someone with the following problem...

A projectile is launched from point A at an angle of 25 degrees relative to the horizontal, with initial velocity = 60 ft/s.
Determine the speed of the projectile along its trajectory where its radius of curvature is 3/4 of its radius of curvature at point A.
(Ignore air resistance.)

We both (independently) worked out a speed = 41.6 m/s, however, the book solution has a speed of 54.5 ft/s.

Appreciate it if someone is able to verify the book's solution.
 
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In general, the radius of curvature of a path is given by ##R=\frac{|\mathbf v|^3}{|\mathbf v\times \mathbf{\dot v}|}##
(where ##\mathbf v## is the velocity along the path and ##\mathbf{ \dot v}## is the acceleration)

In the case of a projectile launched at Earth's surface with speed ##v_0## at an angle θ above the horizontal, (and letting time t=0 be the moment of launch) we have:
##\mathbf v = <v_0\cos\theta, v_0\sin\theta-gt, 0>##
##\mathbf{ \dot v} = <0, -g, 0>##
(I include the third, redundant, component just because the cross product is technically only defined in three dimensions.)

We can thus see that the radius of curvature in this case is proportional to the cube of the speed (specifically ##R=\frac{|\mathbf v|^3}{gv_0\cos\theta}##).
This means that if the curvature becomes 3/4 of the initial curvature, then the speed must become ##\sqrt[3]{3/4}## of the initial speed.

60*(3/4)1/3≈54.5, so the book is indeed correct.

(Notice that we didn't actually need to know the exact launch angle; we only need to know that it wasn't launched straight up.)
 
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