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Question: In the figure shown, two identical blocks each of mass $m$ are connected to three massless springs o...

In the figure shown, two identical blocks each of mass mm are connected to three massless springs of same natural length 'l0l_0' each. If both the blocks are displaced slowly by x0x_0 each from their mean position and released, then the time period of oscillation of each block is T1=2πmaKT_1 = 2\pi \sqrt{\frac{m}{aK}}, when they are oscillating in opposite phase and T2=2πmbKT_2 = 2\pi \sqrt{\frac{m}{bK}} when they are oscillating in same phase, then a×ba \times b = _______.

Answer

9

Explanation

Solution

We have two masses mm connected by three springs: left and right springs each with spring constant KK and a middle spring with spring constant 4K4K.

Step 1. Write the potential energy.

  • Left spring: UL=12Kx12U_L=\frac{1}{2}Kx_1^2.
  • Right spring: UR=12Kx22U_R=\frac{1}{2}Kx_2^2.
  • Middle spring (extension x2x1x_2-x_1): UM=12(4K)(x2x1)2=2K(x2x1)2U_M=\frac{1}{2}(4K)(x_2-x_1)^2 =2K(x_2-x_1)^2.

Step 2. Consider the two normal modes.

  1. In-phase (symmetric) mode:
    Let x1=x2=xx_1=x_2=x. Then
Utotal=12Kx2+12Kx2+2K(0)2=Kx2.U_{\text{total}}=\frac{1}{2}Kx^2+\frac{1}{2}Kx^2 + 2K(0)^2 = Kx^2.

For each block the effective spring constant is KK, so the angular frequency is

ω2=Km,\omega_2 =\sqrt{\frac{K}{m}},

and hence

T2=2πmK.T_2=2\pi\sqrt{\frac{m}{K}}.

Comparing with given T2=2πmbKT_2=2\pi\sqrt{\frac{m}{bK}}, we have b=1b=1.

  1. Opposite-phase (antisymmetric) mode:
    Let x1=xx_1=x and x2=xx_2=-x. Then the middle spring extension becomes
x2x1=xx=2x.x_2-x_1= -x-x=-2x.

So,

UM=2K(2x)2=8Kx2.U_M=2K(2x)^2=8Kx^2.

Now, the side springs contribute:

UL=12Kx2,UR=12Kx2,U_L=\frac{1}{2}Kx^2,\quad U_R=\frac{1}{2}Kx^2,

and the total potential energy is

Utotal=12Kx2+12Kx2+8Kx2=9Kx2.U_{\text{total}} = \frac{1}{2}Kx^2+\frac{1}{2}Kx^2+8Kx^2 =9Kx^2.

The total kinetic energy (since both masses move with speed x˙\dot{x} but in opposite directions) is

T=12mx˙2+12mx˙2=mx˙2.T=\frac{1}{2}m\dot{x}^2+\frac{1}{2}m\dot{x}^2= m\dot{x}^2.

Therefore, the effective spring constant for the mode is 9K9K and the angular frequency is

ω1=9Km.\omega_1=\sqrt{\frac{9K}{m}}.

Thus,

T1=2πm9K.T_1=2\pi\sqrt{\frac{m}{9K}}.

Comparing with T1=2πmaKT_1=2\pi\sqrt{\frac{m}{aK}} we obtain a=9a=9.

Step 3. Calculate:

a×b=9×1=9.a\times b=9\times 1=9.

Explanation (minimal):

  1. For in-phase mode, only side springs act, so b=1b=1.
  2. For opposite-phase mode, energy gives effective constant 9K9K, so a=9a=9.
  3. Thus, a×b=9a \times b = 9.