To solve this problem, we need to use the formula for the period of simple harmonic motion (SHM) of a mass-spring system: \(T = 2\pi \sqrt{\frac{m}{k}}\), where \(T\) is the period, \(m\) is the mass, and \(k\) is the spring constant.
Initially, the period \(T_1 = 1 \, \text{s}\), so:
\(1 = 2\pi \sqrt{\frac{m}{k}}\)
Squaring both sides, we get:
\(\frac{m}{k} = \frac{1}{4\pi^2}\)
When the mass is increased by 3 kg, the new period \(T_2 = 2 \, \text{s}\):
\(2 = 2\pi \sqrt{\frac{m+3}{k}}\)
Squaring both sides, we have:
\(\frac{m+3}{k} = \frac{1}{\pi^2}\)
Now, we have two equations:
(1) \(\frac{m}{k} = \frac{1}{4\pi^2}\)
(2) \(\frac{m+3}{k} = \frac{1}{\pi^2}\)
Subtract equation (1) from equation (2):
\(\frac{3}{k} = \frac{1}{\pi^2} - \frac{1}{4\pi^2}\)
\(\frac{3}{k} = \frac{4 - 1}{4\pi^2}\)
\(\frac{3}{k} = \frac{3}{4\pi^2}\)
Solving for \(k\), we get:
\(k = 4\pi^2\)
Substitute \(k = 4\pi^2\) back into equation (1):
\(\frac{m}{4\pi^2} = \frac{1}{4\pi^2}\)
From which, \(m = 1\) kg.
Thus, the value of the mass \(m\) is \(1\) kg, which is within the given range of 1 to 1.