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Figure 4 shows the structure of a violin and Figure 5 shows a close-up image of the tuning pegs - AQA - A-Level Physics - Question 3 - 2018 - Paper 1

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Figure 4 shows the structure of a violin and Figure 5 shows a close-up image of the tuning pegs. The strings are fixed at end A. The strings pass over a bridge and ... show full transcript

Worked Solution & Example Answer:Figure 4 shows the structure of a violin and Figure 5 shows a close-up image of the tuning pegs - AQA - A-Level Physics - Question 3 - 2018 - Paper 1

Step 1

Explain how a stationary wave is produced when a stretched string is plucked.

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Answer

A stationary wave is produced in a stretched string when it is plucked due to the interaction of two waves traveling in opposite directions. When the string is plucked, waves travel towards the fixed ends and are reflected back. These reflected waves interfere with the incoming waves, creating nodes (points of no displacement) at fixed ends and antinodes (points of maximum displacement) in between. This results in the formation of standing waves characterized by specific frequencies called harmonics.

Step 2

The vibrating length of one of the strings of a violin is 0.33 m.

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Answer

To show that the mass of a 1.0 m length of the string is about 4 × 10^{-4} kg, we can use the relationship between frequency, tension, and linear mass density:

f=12LTμf = \frac{1}{2L} \sqrt{\frac{T}{\mu}}

Where:

  • ff is the frequency (370 Hz),
  • LL is the vibrating length (0.33 m),
  • TT is the tension (25 N), and
  • mu\\mu is the linear mass density of the string.

Rearranging gives us:

μ=T(2Lf)2\mu = \frac{T}{(2Lf)^2}

Substituting the known values:

μ=25(2×0.33×370)24×104 kg/m\mu = \frac{25}{(2 \times 0.33 \times 370)^2} ≈ 4 × 10^{-4} \text{ kg/m}

Thus, for a 1.0 m length, the mass would approximately be 4 × 10^{-4} kg.

Step 3

Determine the speed at which waves travel along the string in question 03.2.

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Answer

The speed of the waves in the string can be determined using the formula:

v=f×λv = f \times \lambda

Where:

  • ff is the frequency (370 Hz), and
  • λ\lambda is the wavelength.

In the case of the first harmonic, the wavelength can be calculated as:

λ=2L=2×0.33=0.66m\lambda = 2L = 2 \times 0.33 = 0.66 \, m

Thus, substituting:

v=370×0.66244.2m/sv = 370 \times 0.66 ≈ 244.2 \, m/s

Step 4

Figure 6 shows how the tension in the string in question 03.2 varies with the extension of the string.

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Answer

From Figure 6, the tension in the string is directly proportional to the extension. When the initial tension is 25 N, and based on the graph, we can determine the tension for different extensions. If the tension increases steadily with extension as shown, the tension will eventually become greater than the original tension as the string is stretched. Therefore, the relationship can be observed through linearity and should remain consistent up to the breaking point.

Step 5

Determine the higher frequency that is produced when the string is stretched by rotating the tuning peg through an angle of 75°.

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Answer

To find the new frequency after rotating the tuning peg, we first calculate the new length of the string assuming the angle of rotation causes an increase in the effective length. The increase in string length is found through:

extra extension=22.5×753603.75 mm\text{extra extension} = 22.5 \times \frac{75}{360} \approx 3.75 \text{ mm}

Then,

  • New length Lnew=0.33+(3.75/1000)=0.33475mL_{new} = 0.33 + (3.75 / 1000) = 0.33475 \, m.

Now using the formula: fnew=12LTμf_{new} = \frac{1}{2L}\sqrt{\frac{T}{\mu}} Using the updated parameters, we can compute the new frequency, which will be greater than the original (greater than 370 Hz). Thus the final value should be determined by calculation.

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