Curvilinear Motion Homework: Normal & Tangential Accel. & Radius

AI Thread Summary
The discussion focuses on calculating the normal and tangential components of acceleration, as well as the radius of curvature for a package dropped from a plane flying at a constant horizontal velocity of 150 ft/s. At the moment of release, the tangential acceleration is zero due to constant horizontal velocity, while the normal acceleration is determined using centripetal acceleration formulas. The radius of curvature at the moment of release is calculated to be approximately 698.758 ft, while just before impact, it is found to be 3900.339 ft. The participants clarify that the gravitational acceleration acts perpendicular to the velocity during the drop. Overall, the calculations emphasize the relationship between velocity, acceleration, and radius of curvature in curvilinear motion.
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Homework Statement



A package is dropped from the plane which is flying with a constant horizontal velocity of va=150 ft/s. Determine the normal and tangential components of acceleration, and the radius of curvature of the path of motion (a) at the moment the package is released at A, (b) just before the package strikes the ground at B.

317a340.png


Homework Equations



s = s_{o} + v_{o}t + (1/2)(a_{t})_{c}t^{2}
v = v_{o} + (a_{t})_{c} t
v^{2} = (vo)^{2} + 2(a_{t})_{c} (s - s_{o})

\rho = \frac{1 + ((\frac{dy}{dx})^{2})^{3/2}}{|d^{2}y/dx^{2}|}

The Attempt at a Solution



s = s_{o} + v_{o}t + (1/2)(a_{t})_{c}t^{2}

x = 0 + (150ft/s)t + 0

x =150t

t = \frac{x}{150}

s = s_{o} + v_{o}t + (1/2)(a_{t})_{c}t^{2}

y = 0 + 0 + (1/2)(-32.2ft/s^{2})t^{2}

y = (-16.1ft/s^{2})t^{2}

y = (-16.1ft/s^{2})(\frac{x}{150})^{2}

y = -0.000716x^{2} This is the equation of the path.

dy/dx = -0.00143x

d^{2}y/dx^{2} = -0.00143

x = 1023.785ft

\rho = \frac{1 + ((\frac{dy}{dx})^{2})^{3/2}}{|d^{2}y/dx^{2}|}

\rho = \frac{1 + (((-0.00143)(1023.785 ft))^{2})^{3/2}}{|-0.00143|}

\rho = 3900.339ft I am assuming this is the \rho for (b).

I am unsure how to get the \rho for (a).

The a_{t} I think for (a) is 0 because the velocity in the horizontal is constant. I am unsure the a_{n} because I need \rho.

I don't understand how to get a_{t} and a_{n} just before it strikes the ground because I don't have a time, do I just assume 1 second before hitting the ground?
 
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Nice work! :cool:

As soon as the package is released, you know the speed and you know that the acceleration is directed towards the center of the circle and is perpendicular to the velocity, i.e. it is centripetal. So ...
 
a_{n} at the moment the package is released

a_{n} = \frac{v^{2}}{\rho}

a_{n} = \frac{(150ft/s)^{2}}{3900.339ft}

a_{n} = 5.769 ft/s^{2}
 
3900 ft/s is the radius of curvature for (b) not (a). When the package is released you know the centripetal acceleration, you don't need to calculate it. Use the known value to find the radius of curvature.
 
Is it gravity?:

a_{n} = \frac{v^{2}}{\rho}

32.2ft/s^{2} = \frac{(150ft/s)^{2}}{\rho}

32.2ft/s^{2} = \frac{(150ft/s)^{2}}{\rho}

\rho = \frac{(150ft/s)^{2}}{32.2ft/s^{2}}

\rho = 698.758 ft
 
Yes it is. Instantaneously at the point of release the package is going around in a circle and the acceleration of gravity is perpendicular to the velocity. You are done.
 
Ok thanks.
 
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