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Question: Two blocks of masses m, and my are kept on a smooth horizontal surface. A spring of mass m and natur...

Two blocks of masses m, and my are kept on a smooth horizontal surface. A spring of mass m and natural leng Lo connects the two blocks as shown in the figure. +=0, m, and my are given velocities v, and 2v as show Just after t = 0, what is the value of x, so that the point remains at rest?

Answer

x=L03\displaystyle x=\frac{L_0}{3}

Explanation

Solution

We choose a coordinate along the unstretched spring of natural length L0L_0 with x=0x=0 at the left end (attached to the block of mass mm given velocity vv) and x=L0x=L_0 at the right end (attached to the other block of mass mym_y given speed 2v2v). (In problems of this type the directions are taken so that one velocity is positive and the other negative. Here we let the left mass move to the right with speed vv and the right mass move to the left with speed 2v2v.)

Immediately after the impulse the spring (having non‐zero mass mm) does not “know” about the impulse at the other end. Thus, while the ends instantaneously acquire the velocities of the blocks, the velocity of points in the spring must vary continuously from one end to the other. (In many elementary texts this is taken as a linear variation along the spring.)

So assume that a point at distance xx (measured from the left end) has velocity

v(x)=v+[vRvLL0]x,v(x)=v +\left[\frac{v_R - v_L}{L_0}\right]\,x,

with

vL=vandvR=(2v)v_L=v\quad\text{and}\quad v_R=(-2v)

(the minus sign comes because the right–end velocity is opposite to the left–end’s direction). Thus

v(x)=v+[2vvL0]x=v3vL0x.v(x)=v +\left[\frac{-2v-v}{L_0}\right]x=v - \frac{3v}{L_0}\,x.

We now require that there be a point on the spring which is at rest (i.e. v(x)=0v(x)=0). Setting

v3vL0x=0,v-\frac{3v}{L_0}\,x=0,

we solve for xx:

3vL0x=vx=L03.\frac{3v}{L_0}\,x=v\quad\Longrightarrow\quad x=\frac{L_0}{3}.

Thus the point located at a distance L03\frac{L_0}{3} from the left end (attached to mass mm) remains at rest instantaneously.

Core Explanation:

Assume a linear velocity distribution along the spring from vv at x=0x=0 to 2v-2v at x=L0x=L_0. Write

v(x)=v3vL0x.v(x)=v-\frac{3v}{L_0}\,x.

Setting v(x)=0v(x)=0 gives x=L0/3x=L_0/3.