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Physics Problems With Solutions Mechanics For Olympiads And Contests Link Free

backward from the cylinder. The cylinder experiences a forward friction force from the plank. : For the plank: For the cylinder (linear): For the cylinder (rotational about center of mass):

2θ̇θ̈=−3gLcosθ⋅θ̇2 theta dot theta double dot equals negative the fraction with numerator 3 g and denominator cap L end-fraction cosine theta center dot theta dot

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Because the string is fixed to the ceiling and does not slip on the cylinder, the kinematic constraint linking translation and rotation is: a=Rα(Equation 3)a equals cap R alpha space (Equation 3) Substitute Equation 3 into Equation 2: T=12Macap T equals one-half cap M a Now, substitute this expression for into Equation 1: Mg−12Ma=Macap M g minus one-half cap M a equals cap M a

, the derivative is positive, meaning the equilibrium is .

ax,cm=ddt(−L2sinθ⋅θ̇)=−L2(cosθ⋅θ̇2+sinθ⋅θ̈)a sub x comma c m end-sub equals d over d t end-fraction open paren negative the fraction with numerator cap L and denominator 2 end-fraction sine theta center dot theta dot close paren equals negative the fraction with numerator cap L and denominator 2 end-fraction open paren cosine theta center dot theta dot squared plus sine theta center dot theta double dot close paren If you are looking to elevate your physics

K=12M(L24θ̇2)+12(112ML2)θ̇2=16ML2θ̇2cap K equals one-half cap M open paren the fraction with numerator cap L squared and denominator 4 end-fraction theta dot squared close paren plus one-half open paren 1 over 12 end-fraction cap M cap L squared close paren theta dot squared equals one-sixth cap M cap L squared theta dot squared By Conservation of Energy (

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Iputty=M(L4)2=116ML2=348ML2cap I sub p u t t y end-sub equals cap M open paren the fraction with numerator cap L and denominator 4 end-fraction close paren squared equals 1 over 16 end-fraction cap M cap L squared equals 3 over 48 end-fraction cap M cap L squared Total moment of inertia: Iputty=M(L4)2=116ML2=348ML2cap I sub p u t t y

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The combined system rotates as a rigid body with angular velocity about the CoM. We must find the new total moment of inertia Itotalcap I sub t o t a l end-sub about this pivot. Using the Parallel Axis Theorem for the rod: