Derive the magnitude and direction of the linear acceleration

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SUMMARY

The discussion focuses on deriving the magnitude and direction of linear acceleration at the tip of a stick, specifically under centripetal motion while ignoring gravity. The key equations utilized include the velocity components vx = rω cos(θ) and vy = rω sin(θ), leading to the acceleration components ax = rω² sin(θ) and ay = -rω² cos(θ). The magnitude of acceleration is confirmed as a = rω², with the direction consistently pointing towards the hinge of the stick, validated through vector analysis.

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  • Understanding of centripetal acceleration concepts
  • Familiarity with angular velocity (ω) and its relationship to linear motion
  • Basic knowledge of vector components and their graphical representation
  • Proficiency in calculus, specifically differentiation (dv/dt)
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  • Explore the implications of centripetal acceleration in circular motion scenarios
  • Study the relationship between angular velocity and linear acceleration in depth
  • Learn about vector analysis techniques for motion in two dimensions
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[Solved] Centripetal Acceleration

Homework Statement


Derive the magnitude and direction of the linear acceleration at the tip of the stick, ignore the effect of gravity.
3047893625_58a74ddb83.jpg


Homework Equations


r = length of stick
a = dv/dt

The Attempt at a Solution


I first find the x and y components of v, then I took the derivative to find ax and ay:

vx = rω cos(θ)
vy = rω sin(θ)

ax = rω ( -sin(θ) dθ/dt ) = rω ( -sin(θ) (-ω) ) = rω2 sin(θ)
ay = rω ( cos(θ) dθ/dt ) = rω ( cos(θ) (-ω) ) = -rω2 cos(θ)

I recognized that ω is -dθ/dt since it is in the opposite direction. This shows that the magnitude of a is rω2. If I were to draw the vector on the graph, it would also show that a is pointing toward the hinge.

But how would I show that a is always pointing toward the hinge?

Is this argument valid:

Let q be the a vector from the tip to the center, then

qx = sin(θ)
qy = -cos(θ)

Now, a • q = rω2cos(ф) = rω2, where ф is the angle between the two vectors and ф=0 in this case. Therefore a and q are in the same direction.

Is there a simpler way to show this?


- Thanks
 
Last edited:
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Your solution is perfect.

Since the components of the acceleration vector are proportional to sin θ and -cosθ, you can also draw a right triangle to show that the acceleration vector points towards the center.
 

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