Calculating Torque and Linear Acceleration of a Rotating Rod

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The discussion revolves around calculating the torque and linear acceleration of a uniform rod pivoted at one end. The torque when the rod is at an angle with the vertical is derived using the formula -Lmg sin(theta)/2, where L is the length of the rod and m is its mass. The participants clarify the relationship between angular and linear acceleration, emphasizing that linear acceleration can be calculated from angular acceleration using the formula a = αr. The correct moment of inertia for the rod pivoted at one end is crucial for solving the problem, leading to the final expression for angular acceleration as α = -3/2(g/L). Ultimately, the linear acceleration at the endpoint is determined to be 14.7 m/s².
  • #31
-1/2Lmg=1/3 M L^2(alpha) ? is this right?
 
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  • #32
ScienceGeek24 said:
-1/2Lmg=1/3 M L^2(w)^2 ?

There's no w^2. Newton's second law for rotation is ##\tau = I \alpha##
 
  • #33
now, how do i cancel the Ls? one has L and the other one has L^2?? even if i manage to cancel them out i don't get the right answer.
 
  • #34
ScienceGeek24 said:
now, how do i cancel the Ls? one has L and the other one has L^2?? even if i manage to cancel them out i don't get the right answer.

You're not done yet. Solve for ##\alpha##. What expression do you get?
 
  • #35
α=-1/2g-1/3L
 
  • #36
ScienceGeek24 said:
α=-1/2g-1/3L

Something went wrong there... You started with

-1/2Lmg=1/3 M L^2(alpha) (assuming m is really M)

How did you end up with two terms? Try that again.
 
  • #37
sorry! i mmeant α=-1/2g/1/3 I got the answer! 14.7 m/s^s thanks man!
 
  • #38
ScienceGeek24 said:
sorry! i mmeant α=-1/2g/1/3 I got the answer! 14.7 m/s^s thanks man!

##\alpha = -\frac{3}{2}\frac{g}{L}##

You've still got the L in the denominator to deal with. It goes away when you calculate the linear acceleration of the endpoint... ##a = \alpha L##.
 
  • #39
oh got it! thanks bro!
 

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