Curvilinear Motion Homework: Normal & Tangential Accel. & Radius

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Homework Help Overview

The problem involves analyzing the motion of a package dropped from a plane traveling at a constant horizontal velocity. The focus is on determining the normal and tangential components of acceleration, as well as the radius of curvature at two specific points: when the package is released and just before it strikes the ground.

Discussion Character

  • Exploratory, Assumption checking, Conceptual clarification

Approaches and Questions Raised

  • Participants discuss the equations of motion and the relationship between velocity, acceleration, and radius of curvature. There is uncertainty regarding how to calculate the radius of curvature at the moment of release and the components of acceleration just before impact.

Discussion Status

Some participants have provided calculations for the radius of curvature and centripetal acceleration, while others question the assumptions made about the acceleration components. There is an acknowledgment of the role of gravity and centripetal acceleration in the analysis, but no consensus on the complete approach for both points in time.

Contextual Notes

Participants are navigating the constraints of the problem, including the need to determine values without explicit time measurements and the implications of constant horizontal velocity on acceleration components.

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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?
 
Last edited:
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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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