How Does Gyroscopic Precession Relate to Torque and Angular Momentum?

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SUMMARY

The discussion focuses on the mathematical relationships between gyroscopic precession, torque, and angular momentum. Key equations include the angular momentum equation \vec{L} = \vec{r} \times \vec{p}, the torque equation \vec{\tau} = \vec{r} \times \vec{F}, and the relationship between angular acceleration and tangential acceleration \alpha = \frac{a_t}{r}. The user seeks clarification on the variables involved in these equations, particularly the meanings of s, \theta, r, \alpha, and a.

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  • Understanding of basic physics concepts such as angular momentum and torque.
  • Familiarity with the equations of motion in circular dynamics.
  • Knowledge of moment of inertia and its role in rotational motion.
  • Basic mathematical skills to manipulate and understand equations.
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Students studying physics, particularly those focusing on mechanics, as well as educators looking to clarify concepts of torque and angular momentum in gyroscopic systems.

cucumber
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hi. not sure if this belongs in here, so sorry in advance for any trouble caused.
i am in a bit of a predicament with a physics assessment of mine; i need to know the mathematical relationships between the precessional frequency, the couple (or torque, as i have read it called) and the angular momentum of a gyroscope, and (here comes the tricky bit) i would like to understand it...
i just need someone to point me in the right direction, i mean i hardly know which questions to ask or where to start looking (sob sob).
i am quasi-familiar with the concept of moment of inertia being the equivalent of mass in linear motion and angular velocity that of velocity (duh), but i have not found a set of formulae that would allow me to make a connection between the aforementioned...er... things...

i come with the rather unsound basis of a-level physics, which is why it will be an especially challenging task for you get me to understand it. good luck (and thanks).

cucumber.
 
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\theta r = s
\omega r = v
\alpha r = a
\vec{L} = \vec{r} \times \vec{p}
\vec{\tau} = \vec{r} \times \vec{F}

cookiemonster
 
thanks cookiemonster.
i'm unsure about a couple of things, though...

what are the "s" and the theta in [theta]*r = s

what are the alpha and the "a" in [alpha]*r = a

what are the "r"'s in both the above equations (just to be sure...)

and finally, what are those two other equations all about?
i suppose that funny looking thing (like half a pi) is torque, but the rest i have absolutely no idea... sorry.
i'd be very grateful if you could clarify them a bit.

thanks again.
cucumber.
 
In a circle of radius r the length of any arc is given by the angle it creates with the center of the circle times the radius: s = \theta r

Angular acceleration:
\alpha = \frac{a_t}{r}
http://hyperphysics.phy-astr.gsu.edu/hbase/rotq.html#rq

Angular momentum:
\vec{L} = \vec{r} \times \vec{p}
http://hyperphysics.phy-astr.gsu.edu/hbase/amom.html

Torque ('tau'):
\vec{\tau} = \vec{r} \times \vec{F}
http://hyperphysics.phy-astr.gsu.edu/hbase/torq2.html#tc

Precession of Gyroscope:
http://hyperphysics.phy-astr.gsu.edu/hbase/gyr.html#gyr
 

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