To find the fundamental frequency of a vibrating wire, we use the formula for the fundamental frequency of a string fixed at both ends:
f = \(\frac{1}{2L}\) \(\sqrt{\frac{T}{\mu}}\)
Where:
Substitute these values into the formula:
f = \(\frac{1}{2 \times 0.5}\) \(\sqrt{\frac{4}{0.0001}}\)
f = \(\frac{1}{1}\) \(\sqrt{40000}\)
The square root of 40000 is 200, so:
f = 200 Hz
Hence, the fundamental frequency of the wire is 200 Hz.
The fundamental frequency \( f_1 \) of a vibrating string is given by: \[ f_1 = \frac{1}{2L} \sqrt{\frac{T}{\mu}} \] where:
- \( L = 0.5 \, \text{m} \),
- \( T = 4 \, \text{N} \),
- \( \mu = 0.0001 \, \text{kg/m} \). Substitute the values into the equation: \[ f_1 = \frac{1}{2 \times 0.5} \sqrt{\frac{4}{0.0001}} = \frac{1}{1} \times \sqrt{40000} = 200 \, \text{Hz} \] Thus, the fundamental frequency is 200 Hz.
A stretched wire fixed at both ends supports transverse waves that travel along it with speed \( v = \sqrt{T/\mu} \), where \(T\) is the tension and \(\mu\) is the mass per unit length. For the fundamental (first) mode, the wire's full length \(L\) holds exactly half a wavelength, so \( \lambda = 2L \), and the frequency is \( f = v/\lambda \). With \( T = 4\,\text{N} \) and \( \mu = 0.0001\,\text{kg/m} \), \( v = \sqrt{4/0.0001} = \sqrt{40000} = 200\,\text{m/s} \), and with \( L = 0.5\,\text{m} \), \( \lambda = 1\,\text{m} \), giving \( f = 200/1 = 200\,\text{Hz} \). Let's check the options against this.
The wave speed set by the tension and mass per unit length, divided by the fundamental wavelength of twice the wire's length, gives 200 Hz.
So the correct answer is 200 Hz.