Spiral Moment

x = θ cos ( θ ) y = θ sin ( θ ) 0 θ 4 3 x = \theta\cos(\theta)\hspace{1cm}y=\theta\sin(\theta)\hspace{1cm}0\leq\theta\leq4\sqrt{3}

The spiral object described above exists in the x y xy plane and has a linear mass density ( σ = 1 θ ) (\sigma =\Large{\frac{1}{\theta}}) .

Determine the object's moment of inertia with respect to an axis perpendicular to the x y xy plane and passing through the point ( x , y ) = ( 0 , 0 ) (x,y) = (0,0) .

Details and Assumptions: All angles are in radians


The answer is 114.

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2 solutions

Steven Chase
Sep 11, 2016

Here's another look at why the differential change in arc length is not simply equal to r d θ r\, d\theta .

exactly same as me !! :)

A Former Brilliant Member - 4 years, 5 months ago

In polar form this equation is r=∅ So dL=rd∅-------for certain ∅ dm=Sigma*dl=d∅ Moment of inertia= integral r²dm =∅²d∅ from ∅ =0 to ∅=4√3 Which yields answer as 64√3 which is 110.85 Why are the two answers different?

Hrushikeshcoc Bodas - 4 years, 8 months ago

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Hello. I believe the answer is that the differential arc length dL is only equal to r * d(theta) in certain cases, such as a circle. I have supplemented my original solution with some additional derivations confirming this. Please have a look at it.

Steven Chase - 4 years, 8 months ago

the general form for moment of inertia is d m x 2 \int dm*x^2 where x x is a parameter , it is obvious from the quesion given that here it is θ \theta and from here on..... find the arclength and it's small mass, integrate over the limits .. ..i have to say the limits are awesome as i was afraid how the answer will come out to be integer .... steven sir has alrady given pictorial solutions as i usually do ! nice one sir ..! the answer is 343/3-1/3 = 342/3 =114 answer !

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