Question

Difficulty: MediumResononace, Vibrating Strings, and Air Columns in Pipes

A uniform wire of length 0.60 m0.60\text{ m} fixed at both ends vibrates in its fundamental mode with a frequency of 150 Hz150\text{ Hz}. If the length of the wire is reduced to 0.40 m0.40\text{ m} while the tension in the wire is increased by a factor of 4, what is the new fundamental frequency of vibration?

  1. A
    200 Hz200\text{ Hz}
  2. B
    300 Hz300\text{ Hz}
  3. 450 Hz450\text{ Hz}Answer
  4. D
    900 Hz900\text{ Hz}

Answer

The new fundamental frequency of the vibrating wire is 450 Hz450\text{ Hz}.
The fundamental frequency of a stretched string is inversely proportional to its length and directly proportional to the square root of its tension (fTLf \propto \frac{\sqrt{T}}{L}). Reducing the length from 0.60 m0.60\text{ m} to 0.40 m0.40\text{ m} increases frequency by a factor of 0.600.40=1.5\frac{0.60}{0.40} = 1.5. Quadrupling the tension increases frequency by a factor of 4=2\sqrt{4} = 2. Combining both effects gives an overall frequency multiplier of 1.5×2=3.01.5 \times 2 = 3.0, leading to 3.0×150 Hz=450 Hz3.0 \times 150\text{ Hz} = 450\text{ Hz}.

Step-by-Step Solution

1
Write the general formula for the fundamental frequency of a stretched string.
f=12LTμf = \frac{1}{2L} \sqrt{\frac{T}{\mu}}, where LL is length, TT is tension, and μ\mu is linear density.
Establishes the functional dependence of frequency on length and tension.
2
Set up the ratio between the new frequency f2f_2 and initial frequency f1f_1.
f2f1=L1L2T2T1\frac{f_2}{f_1} = \frac{L_1}{L_2} \sqrt{\frac{T_2}{T_1}}.
Since linear mass density μ\mu remains constant, comparing ratios isolates the changing variables.
3
Substitute the given parameters into the ratio equation.
f2150=0.600.40×4=1.5×2=3.0\frac{f_2}{150} = \frac{0.60}{0.40} \times \sqrt{4} = 1.5 \times 2 = 3.0.
Calculates the scaling factor for the new fundamental frequency.
4
Solve for the new fundamental frequency f2f_2.
f2=3.0×150=450 Hzf_2 = 3.0 \times 150 = 450\text{ Hz}.
Yields the final numerical value of the modified fundamental frequency.

Key Concept

Fundamental frequency of vibrating stretched strings under varying length and tension
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