Question #168036

Two bodies m1 and m2 attached to each other by weightless rigid rod of length a can slide along fixed axes which formed angle with horizontal axis (as drawn shows). Find the Lagrangian of this system?


Expert's answer

Let the kinetic energy of each block be T1T_1 and T2T_2

Total energy of the system be T=T1+T2T=T_1+T_2

T1=m1v22T_1=\frac{m_1v2}{2}


T2=m2v22T_2=\frac{m_2 v^2}{2}


x=lsin⁡θcos⁡ϕ2x=\frac{l\sin\theta\cos\phi}{2}


y=lsin⁡θcos⁡ϕ2y=\frac{l\sin\theta\cos\phi}{2}

Now, taking the differentiation,

x˙2+y˙2+z˙2=v2....(i)\dot{x}^2+\dot{y}^2+\dot{z}^2=v^2 ....(i)


x˙=l2(cos⁡ϕcos⁡θθ˙−sin⁡θsin⁡ϕϕ˙)\dot{x}=\frac{l}{2}(\cos\phi \cos\theta\dot{\theta}-\sin\theta\sin\phi \dot{\phi})


y˙=l2(sin⁡ϕcos⁡θθ˙−sin⁡θcos⁡ϕϕ˙)\dot{y}=\frac{l}{2}(\sin\phi \cos\theta\dot{\theta}-\sin\theta\cos\phi \dot{\phi})


z˙=−l2sin⁡θθ˙\dot{z}=-\frac{l}{2}\sin\theta \dot{\theta}

Now, substituting the values in (i)

⇒x˙2+y˙2+z˙2=l24(cos⁡2ϕcos⁡2θθ˙2+sin⁡2ϕsin⁡2θϕ˙2+sin⁡2ϕcos⁡2θθ˙2−sin⁡2θcos⁡2ϕϕ˙2+sin⁡2θθ˙2)\Rightarrow \dot{x}^2+\dot{y}^2+\dot{z}^2=\frac{l^2}{4}(\cos^2\phi \cos^2\theta\dot{\theta}^2+\sin^2\phi \sin^2\theta\dot{\phi}^2+\sin^2\phi \cos^2\theta\dot{\theta}^2-\sin^2\theta\cos^2\phi \dot{\phi}^2+\sin^2\theta\dot{\theta}^2)

v2=l24(θ˙2+sin⁡2θϕ˙2)v^2=\frac{l^2}{4}(\dot{\theta}^2+\sin^2\theta\dot{\phi}^2)

Now, substituting the value of v2=ma2ψ˙2+ml24(θ˙2+sin⁡2θϕ˙2)v^2=ma^2\dot{\psi}^2+\frac{ml^2}{4}(\dot{\theta}^2+\sin^2\theta\dot{\phi}^2)

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