Very basic question on particle dynamics

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Homework Help Overview

The discussion revolves around a problem in particle dynamics involving a car making a left turn from a stopped position, with a focus on the forces acting on a book on the dashboard as the car accelerates. The problem includes concepts of friction, circular motion, and acceleration.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants explore the relationship between tangential and centripetal acceleration and how they affect the motion of the book. There are attempts to clarify the role of friction in preventing the book from sliding and questions about the calculations leading to differing results.

Discussion Status

Participants are actively engaging with the problem, questioning assumptions about the effects of centripetal acceleration and discussing the need to consider both components of acceleration. Some guidance has been offered regarding the relationship between the forces and accelerations involved.

Contextual Notes

There is mention of differing answers between the original poster and the teacher, indicating potential confusion or misinterpretation of the problem setup. The discussion also highlights the need for clarity on the application of equations related to circular motion and friction.

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Homework Statement


A car makes a left turn from a stopped position, increasing its speed at a rate of 2 m/s/s. If a book is on the dashboard of the car, at what time will the book begin to slide if the static coefficient of friction \mu_s = 0.3? The radius of the curve of the motion is 7m.

Seems straight forward enough but the answer I get is different to the one my teacher put in the tutorial sheet, and would just like a 2nd opinion on this to make sure I'm not going mad.

Homework Equations


Normal force on a particle in circular motion: F_n = m\frac{v^2}{R}
Maximum frictional force between the box and dash board: F_f = N\mu_s = mg \mu_s
Constant acceleration equations: v = v_0 + at

The Attempt at a Solution


Let the book have mass m. Just as the book is about to slide: F_f = F_n \implies m\frac{v^2}{R} = m\frac{(at)^2}{R} = mg \mu_s \implies t = \frac{\sqrt{gR\mu_s}}{a}

Plugging in the numbers, I get t\approx 2.27 \text{s} whereas my teacher's put t= 1.94\text{s}

Thanks for the help.
 
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Don't forget there are two components of the acceleration. There's the radial (centripetal) acceleration that you have calculated above in your original post.

But there is also the tangential acceleration (2 m/s2) that acts at a right angle relative to the radial acceleration.

You can find the total acceleration's magnitude by finding the hypotenuse.
 
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collinsmark said:
Don't forget there are two components of the acceleration. There's the radial (centripetal) acceleration that you have calculated above in your original post.

But there is also the tangential acceleration (2 m/s2) that acts at a right angle to the radial acceleration.

You can find the total acceleration's magnitude by finding the hypotenuse.
But surely the centripetal acceleration has no effect on the magnitude of the book's tangential velocity (speed)? So the constant acceleration equation still applies to calculate the book's speed, which in turn can be used to calculate the magnitude of the centripetal force, which the frictional force between the book and the dashboard needs to match to prevent it from sliding, no?
 
TomW17 said:
But surely the centripetal acceleration has no effect on the magnitude of the book's tangential velocity (speed)? So the constant acceleration equation still applies to calculate the particle's speed, which in turn can be used to calculate the magnitude of the centripetal force?

Yes, go ahead and use your |v| = |a_t|t equation to find the book's speed (that's the way it was specified in the problem statement, in less specific variables). And like you've already done, you can use a_r = \frac{v^2}{R}, as you have done.

But then note that the overall acceleration magnitude is the magnitude of the two acceleration vectors forming a right triangle.
 
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collinsmark said:
Yes, go ahead and use your |v| = |a_t|t equation to find the book's speed (that's the way it was specified in the problem statement, in less specific variables). And like you've already done, you can use a_r = \frac{v^2}{R}, as you have done.

But then note that the overall acceleration magnitude is the magnitude of the two acceleration vectors forming a right triangle.
Aha, got it, completely neglected that the frictional force accelerates the book tangentially as well as keeps it in circular motion. Thanks very much.
 
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