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Question: Rod A of mass m, length $l$ and coefficient of thermal coefficient $\alpha$ is joined with Rod B of ...

Rod A of mass m, length ll and coefficient of thermal coefficient α\alpha is joined with Rod B of mass 2m, length ll and coefficient of thermal expansion α3\frac{\alpha}{3}. Rods are kept on smooth floor. If temperature of rods is increased by ΔT\Delta T, then junction of the rods shifts by distance αlΔTn\frac{\alpha l \Delta T}{n}, Find value of n.

Answer

18

Explanation

Solution

Solution:

Let the initial positions be such that rod A extends from 0 to ll (with mass mm) and rod B from ll to 2l2l (with mass 2m2m). When heated by ΔT\Delta T:

  1. Expansion of lengths:

    • Rod A expands from ll to lA=l(1+αΔT).l_A = l(1+\alpha\Delta T).
    • Rod B expands from ll to lB=l(1+α3ΔT).l_B = l\left(1+\frac{\alpha}{3}\Delta T\right).
  2. Displacements:

    Let uu be the displacement of the free (left) end of rod A, ss the displacement of the junction (which is common to both rods) and vv the displacement of the free (right) end of rod B. Then

    su=l+αlΔT(rod A)s - u = l + \alpha l\Delta T \quad \text{(rod A)}

    and

    vs=l+αlΔT3(rod B).v - s = l + \frac{\alpha l\Delta T}{3} \quad \text{(rod B)}.
  3. Conservation of center of mass (COM):

    Since the floor is smooth, no external horizontal force acts; hence the overall COM remains fixed. The new COM positions of the rods (being uniform) are the averages of their endpoints:

    COMA=u+s2,COMB=s+v2.\text{COM}_A = \frac{u+s}{2},\quad \text{COM}_B = \frac{s+v}{2}.

    The overall COM of the system (total mass 3m3m) must equal its initial value:

    m(u+s)2+2m(s+v)23m=constant.\frac{m\frac{(u+s)}{2} + 2m\frac{(s+v)}{2}}{3m} = \text{constant}.

    Initially, COM of rod A is l2\frac{l}{2} and rod B is 3l2\frac{3l}{2}, so overall COM is:

    ml2+2m3l23m=l2+3l3=7l6.\frac{m\frac{l}{2} + 2m\frac{3l}{2}}{3m} = \frac{\frac{l}{2}+3l}{3} = \frac{7l}{6}.
  4. Expressing endpoints in terms of ss:

    From the expansion conditions:

    u=s(l+αlΔT),u = s - \left(l+\alpha l\Delta T\right), v=s+(l+αlΔT3).v = s + \left(l+\frac{\alpha l\Delta T}{3}\right).
  5. Setting up COM conservation:

    The new overall COM is

    16[(u+s)+2(s+v)]=16[(s(l+αlΔT)+s)+2(s+s+l+αlΔT3)].\frac{1}{6}\left[(u+s) + 2(s+v)\right] = \frac{1}{6}\Bigl[ \bigl(s - (l+\alpha l\Delta T) + s\bigr) + 2\Bigl(s+s + l+\frac{\alpha l\Delta T}{3}\Bigr)\Bigr].

    Simplify step‐by‐step:

    u+s=2s(l+αlΔT),u+s = 2s - \left(l+\alpha l\Delta T\right), 2(s+v)=2(2s+l+αlΔT3)=4s+2l+2αlΔT3.2(s+v) = 2\left(2s + l+\frac{\alpha l\Delta T}{3}\right) = 4s + 2l + \frac{2\alpha l\Delta T}{3}.

    Therefore,

    New COM=6s+lαlΔT36=s+l6αlΔT18.\text{New COM} = \frac{6s + l - \frac{\alpha l\Delta T}{3}}{6} = s + \frac{l}{6} - \frac{\alpha l\Delta T}{18}.

    Equating to the initial COM:

    s+l6αlΔT18=7l6.s + \frac{l}{6} - \frac{\alpha l\Delta T}{18} = \frac{7l}{6}.

    Solve for ss:

    s=7l6l6+αlΔT18=l+αlΔT18.s = \frac{7l}{6} - \frac{l}{6} +\frac{\alpha l\Delta T}{18} = l + \frac{\alpha l\Delta T}{18}.
  6. Junction shift:

    The junction originally was at x=lx=l and now is at

    s=l+αlΔT18.s = l + \frac{\alpha l\Delta T}{18}.

    So the shift is

    Δx=αlΔT18.\Delta x = \frac{\alpha l\Delta T}{18}.

    Comparing with the given form αlΔTn\frac{\alpha l\Delta T}{n}, we identify

    n=18.n = 18.

Explanation (minimal):

  • Write expansion conditions: su=l+αlΔTs-u = l+\alpha l\Delta T and vs=l+αlΔT3v-s = l+\frac{\alpha l\Delta T}{3}.
  • Express endpoints uu and vv in terms of ss.
  • Use COM conservation: (u+s)+2(s+v)6=7l6.\frac{(u+s) + 2(s+v)}{6} = \frac{7l}{6}.
  • Solve to obtain s=l+αlΔT18s = l + \frac{\alpha l\Delta T}{18}.
  • Thus, junction shift =αlΔT18=\frac{\alpha l\Delta T}{18} implying n=18n=18.