91Ó°ÊÓ

• Original spring constant,k=8600 N/m .
• The length of two pieces, ${\mathrm{L}}_1=7.0\mathrm{cm}\mathrm{and}{\mathrm{L}}_2=10.0\mathrm{cm}$.
• Original frequency of oscillations,f =200 Hz .

When spring is cut into pieces, the spring constants of the pieces are inversely proportional to the length of the piece. Using the formula for the resultant force constant for the series combination of the spring, we can calculate the force constants and new frequencies of the springs.

Formula:

The spring constant relation to the length of the spring,$k\mathrm{Î\pm }\frac{1}{L}$ (i)

The angular frequency of the spring,

$$\begin{gathered} \mathrm{Ó\neg }=2\mathrm{Ï„}\mathrm{Ï„}f \\ =\sqrt{\frac{k}{m}} \end{gathered}$$ (ii)

Here,

$\mathrm{Ó\neg }$is angular frequency

$f$is frequency

$k$is force constant

$m$is mass

Using condition (i), we get the spring constants of two pieces as:

So, we can write,$k_1\mathrm{Î\pm }\frac{1}{L_1}$ and$K_2\mathrm{Î\pm }\frac{1}{L_2}$

Taking ratio, we get

$$\begin{gathered} \frac{k_2}{k_1}=\frac{L_1}{L_2} \\ =\frac{7.0}{10.0} \\ {k}_2=0.7k_1.....................\left(1\right) \end{gathered}$$

Now, when the two pieces were connected together end to end, the arrangement is called as a series. Hence, the three spring constants (original and two new) are related as

$\frac{1}{k}=\frac{1}{k_1}+\frac{1}{k_2}$

Substituting the value of equation (1), we get the value of spring constant of piece 1 as:
role="math" localid="1657274770042" $$\begin{gathered} \frac{1}{k}=\frac{1}{k_1}+\frac{1}{0.7k_1} \\ =\frac{1.7k}{0.7k_1} \end{gathered}$$

Thus, we get,

$$\begin{gathered} k_1=\frac{1.7k}{0.7} \\ =\frac{1.7×8600}{0.7} \\ =20,886\mathrm{N}/\mathrm{m} \end{gathered}$$

Hence, the value of the spring constant is 20,886 N/m .

And the spring constant from equation (1), we get the spring constant of piece 2 as:

$$\begin{gathered} k_2=0.7k_1 \\ =14,620\mathrm{N}/\mathrm{m} \end{gathered}$$

Hence, the value of the spring constant is 14,620 N/m .

From equation (ii), the frequency of oscillations of the block when attached to piece 1 and 2 can be given as:

$$\begin{gathered} f_1=\frac{1}{2\mathrm{Ï„}\mathrm{Ï„}}\sqrt{\frac{k_1}{m}} \\ {f}_2=\frac{1}{2\mathrm{Ï„}\mathrm{Ï„}}\sqrt{\frac{k_2}{m}} \end{gathered}$$

Taking ratio with respect to the original frequency of oscillations, we get

$$\begin{gathered} \frac{f_1}{f}=\sqrt{\frac{k_1}{m}×\frac{m}{k}} \\ =\sqrt{\frac{k_1}{k}}..............................................\left(a\right) \end{gathered}$$

Hence, we determine the frequency of piece 1 as:
$$\begin{gathered} f_1=f\sqrt{\frac{k_1}{k}} \\ =200\sqrt{\frac{1.7}{0.7}} \\ =312\mathrm{Hz} \end{gathered}$$

Hence, the required value of frequency is 312 Hz .

Similarly, the frequency ratio for piece 2 using equation (a) can be given as:

$$\begin{gathered} \frac{f_2}{f}=\sqrt{\frac{k_1}{k}} \\ {f}_2=f\sqrt{\frac{k_2}{k}} \\ =200\sqrt{1.7} \\ =260\mathrm{Hz} \end{gathered}$$

Hence, the value of required frequency is 260 Hz .