91Ó°ÊÓ

We are given the total mass and length of the wire, so we can calculate the linear mass density of the wire using its definition: \(\mu = \frac{m}{L}\), where \(\mu\) is the linear mass density, \(m\) is the total mass of the wire, and \(L\) is the length of the wire. \(\mu = \frac{3 \mathrm{~kg}}{10 \mathrm{~m}} = 0.3 \mathrm{~\frac{kg}{m}}\)

As we go to the upper end of the wire, the tension decreases as less mass needs to be supported. At the upper end, only the block of mass 1 kg is suspended, so the tension in the wire can be calculated as: \(T_\text{upper} = m_\text{block} \cdot g\), where \(m_\text{block}\) is the mass of the block, which is 1 kg, and \(g\) is the acceleration due to gravity, which is \(9.8 \mathrm{~\frac{m}{s^2}}\). \(T_\text{upper} = 1 \mathrm{~kg} \cdot 9.8 \frac{\mathrm{m}}{\mathrm{s^2}} = 9.8 \mathrm{~ N}\)

Now that we know the tension and linear mass density of the wire at the upper end, we can use the wave speed formula to find the speed of the wave at the upper end: \(v_\text{upper} = \sqrt{\frac{T_\text{upper}}{\mu}}\) \[v_\text{upper} = \sqrt{\frac{9.8 \mathrm{~N}}{0.3 \mathrm{~\frac{kg}{m}}}} = \sqrt{32.67 \frac{\mathrm{m^2}}{\mathrm{s^2}}} \approx 5.72 \frac{\mathrm{m}}{\mathrm{s}}\]

Since the frequency of the wave does not change as it travels through the wire, we can use the known speed and wavelength at the lower end of the wire to find the frequency, using the formula: \(v = f \lambda\), where \(v\) is the speed of the wave, \(f\) is the frequency of the wave, and \(\lambda\) is the wavelength of the wave. We are given the wavelength at the lower end of the wire as 0.05 m, and we know that at the lower end, the wave supports both the block of mass 1 kg and the entire wire of mass 3 kg. So, the tension at the lower end is: \(T_\text{lower} = (m_\text{block} + m) \cdot g = (1 \mathrm{~kg} + 3 \mathrm{~kg}) \cdot 9.8 \frac{\mathrm{m}}{\mathrm{s^2}} = 39.2 \mathrm{~ N}\) Now, we can find the speed of the wave at the lower end: \(v_\text{lower} = \sqrt{\frac{T_\text{lower}}{\mu}} = \sqrt{\frac{39.2 \mathrm{~N}}{0.3 \mathrm{~\frac{kg}{m}}}} = 10 \frac{\mathrm{m}}{\mathrm{s}}\) And then, calculate the frequency using the given wavelength and the calculated speed: \(f = \frac{v_\text{lower}}{\lambda} = \frac{10 \frac{\mathrm{m}}{\mathrm{s}}}{0.05 \mathrm{~m}} = 200 \mathrm{~Hz}\)

Now that we know the frequency and the speed of the wave at the upper end of the wire, we can use the wave speed formula again to find the wavelength \(\lambda_\text{upper}\) at the upper end: \(v_\text{upper} = f \lambda_\text{upper}\) \[\lambda_\text{upper} = \frac{v_\text{upper}}{f} = \frac{5.72 \frac{\mathrm{m}}{\mathrm{s}}}{200 \mathrm{~Hz}} = 0.0286 \mathrm{~m}\] However, this is not an answer choice. When solving these types of problems, we need to consider the fact that in the multiple-choice format, the answer choices are often rounded. In this case, we can round our answer to \(\lambda_\text{upper} \approx 0.03 \mathrm{~m}\), which corresponds to answer choice (C) \(0.03 \mathrm{~m}\).