Two blocks of mass and M connected by a massless spring of spring con stant & are placed on a smooth horizontal table. Determine the equations of
motion using Newtonian mechanics
Answer
The kinetic energy and potential energy from the coupling spring constant k for this system can written as
"T= \\frac1{2} m \nx\n\u02d9\n \n2\n + \\frac1{2} M \ny\n\u02d9\n\u200b\t\n \n2"
And
"V=\\frac1{2}k(x\u2212y) ^2"
So lagrangial of this system can witten as
"L=\\frac1{2} m \nx\n\u02d9\n \n2\n + \\frac1{2} M \ny\n\u02d9\n\u200b\t\n \n2-\\frac1{2}k(x\u2212y) ^2"
Now calculating as below
"\\frac{\\partial L}{\\partial \\dot{x}}=m\\dot{x}, \\\\ \\frac{\\partial L }{\\partial x}=-k(x-y)\\\\ \n \\frac{\u2202L}{\u2202 \nx}\n\u02d9\n =m \nx\n\u02d9\n ,\\\\\u2202L\/\u2202x=\u2212k(x\u2212y)\\\\ \n\n\\partial L \/ \\partial \\dot{y}=M \\dot{y} , \\\\ \\partial L\/ \\partial y=k(x-y)\\\\\u2202L\/\u2202 \ny\n\u02d9\n\u200b\t\n =M"
Now lagrangian equation of motion is given by
"\\frac{d}{dt}{\\frac{\\partial L}{ \\partial \\dot{x}}}-\\frac{\\partial L}{\\partial x}=0, \\\\"
"\\frac{d}{dt}{\\frac{\\partial L}{ \\partial \\dot{y}}}-\\frac{\\partial L}{\\partial y}=0,"
Putting all values then we get
Equation of motion
"m\\ddot{x}+k(x-y)=0\\\\m\\ddot{y}+k(y-x)=0"
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