Centripetal acceleration geometry

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SUMMARY

The discussion focuses on proving the relationship \(\Delta V/V = s/R\) in uniform circular motion, where \(s\) represents the arc length, \(R\) is the radius, and \(\Delta V\) is the change in velocity. The user attempts to demonstrate that the segment \(S\) forms a right triangle with \(\Delta V\) when vectorially adding velocities \(V_1\) and \(V_2\). Key formulas discussed include \(s = R \cdot \phi\) and \(\Delta V = V \cdot \sin(\phi')\), where \(\phi\) and \(\phi'\) are angles in radians. The inscribed angle theorem is referenced to establish that a right angle is formed when the angle subtends a diameter.

PREREQUISITES
  • Understanding of uniform circular motion
  • Familiarity with basic trigonometry and right triangles
  • Knowledge of the inscribed angle theorem
  • Ability to work with angular measurements in radians
NEXT STEPS
  • Study the inscribed angle theorem in detail
  • Explore the relationship between arc length and angle in radians
  • Practice vector addition of velocities in circular motion
  • Investigate the implications of small angle approximations in trigonometry
USEFUL FOR

Students and educators in physics and geometry, particularly those focusing on circular motion and vector analysis. This discussion is beneficial for anyone looking to deepen their understanding of the geometric principles underlying uniform circular motion.

richardbsmith
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This is probably a geometry question more that a physics question. I am trying to prove that in uniform circular motion \Delta V/V= s/R.

I am basically trying to show that S forms a right triangle with \DeltaV, when V{1} is added to V{2} as a vector. (This is to demonstrate that the triangles are similar.)

I understand that the angle formed by S and \DeltaV is a right angle because it obviously inscribes the diameter. I just cannot seem to find a satisfactory proof that \DeltaV must necessarily intersect the circle at the diameter.

Probably not explaining this very well.
 
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richardbsmith said:
This is probably a geometry question more that a physics question. I am trying to prove that in uniform circular motion \Delta V/V= s/R.

I am basically trying to show that S forms a right triangle with \DeltaV, when V{1} is added to V{2} as a vector. (This is to demonstrate that the triangles are similar.)

I understand that the angle formed by S and \DeltaV is a right angle because it obviously inscribes the diameter. I just cannot seem to find a satisfactory proof that \DeltaV must necessarily intersect the circle at the diameter.

Probably not explaining this very well.
If you are solving geometry problems with both distances and velocities involved, then you
are probably making a mistake: remember that they have different units! (unless you study relativistic theory)
For the mentioned problem you should use formulas:
s=R*fi (fi is angle of the part of orbit traveled in radians)
\DeltaV=V*sin(fi') (fi' is the angle between the old and new velocity vector)

Prove that fi=fi' and use sin(fi)=fi (for small angles) and you will get \Delta V/V= s/R
 
Thank you so much for responding. I think though my question which started with uniform motion and delta V, is now simply a geometry question.

I will try to put up a drawing of what I so pitifully tried to explain.

uniformcircularmotion.png


Here is another image with a different angle and size of the tangents.
uniformcircularmotion2.png


I have tried several approaches, but I cannot prove that the angle formed from tangent 1 to tangent 2 to the circle must inscribe a 180 degree arc and must be a right angle.
 
From : http://en.wikipedia.org/wiki/Inscribed_angle_theorem
In geometry, the inscribed angle theorem states that an angle θ inscribed in a circle is half of the central angle 2θ that subtends the same arc on the circle.
So, to get an inscribed angle of 90° you need a central angle of 180°(=diameter line).
 

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