Falling chimney internal torque

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SUMMARY

The discussion centers on the mechanics of a falling chimney and the calculation of internal torque. The equation derived is internal torque + external torque = (mx^2)(3gcosA/2L), where A is the angle with the ground, m is mass, and L is chimney length. The internal torque is maximized at x = L/3, but doubts arise regarding whether maximizing internal force instead of torque is more appropriate. The complexity of determining the breaking point of the chimney is acknowledged, emphasizing the need for simplifying assumptions regarding shear forces, compression, and torque.

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dEdt
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Suppose a (uniform) chimney began falling. Where would the chimney break? I approached the problem by considering the torque acting on a point along the chimney, at a distance x from the point of rotation. I got the internal torque + external torque = (mx^2)(3gcosA/2L), where A is the angle between the chimney and the ground, m is the mass of the point, and L is the length of the chimney. The external torque is just mgcosA; using this, I get that the internal torque is maximized at x = L/3. This, at least, was the given solution. But thinking some more, I began doubting my solution. Shouldn't I be trying to maximize the internal force rather than the internal torque? But doing that yields silly answers, so that seems wrong too. Help please!
 
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Figuring out exactly how a chimney would break would be an extremely complicated problem! To solve it--as you clearly know--you have to make simplifying assumptions.
For instance, you have to guess why it would break--i.e. from shear forces? compression? expansion? torque?

Conceptually, torque seems like a good bet--i.e. the chimney would snap, in which case your analysis is great.
 
I can't see why torque would make it snap though. So what if the torque is maximized there? Worse still, the second derivative is actually positive at x = L/3, so I think it's a minimum in actuality.
 

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