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Figure 1 shows an arrangement used by a student to investigate vibrations in a stretched nylon string of fixed length l - AQA - A-Level Physics - Question 2 - 2017 - Paper 1

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Figure 1 shows an arrangement used by a student to investigate vibrations in a stretched nylon string of fixed length l. He measures how the frequency f of first-har... show full transcript

Worked Solution & Example Answer:Figure 1 shows an arrangement used by a student to investigate vibrations in a stretched nylon string of fixed length l - AQA - A-Level Physics - Question 2 - 2017 - Paper 1

Step 1

Show that the data in Table 1 are consistent with the relationship $f \propto \sqrt{T}$

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Answer

To verify the given relationship, we will calculate the tension TT for each mass using the formula:

T=mgT = mg

where mm is the mass and gg is the acceleration due to gravity (approximately 9.81 m/s29.81 \text{ m/s}^2). For each mass from Table 1:

  • For m=0.50m = 0.50 kg:
    T=0.50×9.81=4.905 NT = 0.50 \times 9.81 = 4.905 \text{ N}
  • For m=0.80m = 0.80 kg:
    T=0.80×9.81=7.848 NT = 0.80 \times 9.81 = 7.848 \text{ N}
  • For m=1.20m = 1.20 kg:
    T=1.20×9.81=11.772 NT = 1.20 \times 9.81 = 11.772 \text{ N}

Next, we will calculate the square root of the tension:

  • For T=4.905T = 4.905:
    T=4.9052.22\sqrt{T} = \sqrt{4.905} \approx 2.22
  • For T=7.848T = 7.848:
    T=7.8482.80\sqrt{T} = \sqrt{7.848} \approx 2.80
  • For T=11.772T = 11.772:
    T=11.7723.43\sqrt{T} = \sqrt{11.772} \approx 3.43

Now, we will determine the ratio of frequencies to the square roots of the tensions:

  • For m=0.50m = 0.50 kg:
    fT=1102.2249.55\frac{f}{\sqrt{T}} = \frac{110}{2.22} \approx 49.55
  • For m=0.80m = 0.80 kg:
    fT=1402.8050.00\frac{f}{\sqrt{T}} = \frac{140}{2.80} \approx 50.00
  • For m=1.20m = 1.20 kg:
    fT=1703.4349.54\frac{f}{\sqrt{T}} = \frac{170}{3.43} \approx 49.54

Since the ratios are approximately the same, the data is consistent with the relationship fTf \propto \sqrt{T}.

Step 2

Determine the length l of the string used.

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Answer

To find the length ll of the string used, we start with the formula relating the tension TT, the mass per unit length μ\mu, and the frequency ff:

f=12lTμf = \frac{1}{2l} \sqrt{\frac{T}{\mu}}

Here, we know that:

  • The density of the string is 1150 kg/m31150 \text{ kg/m}^3.
  • The diameter of the string is 5.0×103 m5.0 \times 10^{-3} \text{ m}.

First, we calculate the cross-sectional area AA of the string:

A=π(d2)2=π(5.0×1032)21.9635×105 m2A = \pi \left(\frac{d}{2}\right)^2 = \pi \left(\frac{5.0 \times 10^{-3}}{2}\right)^2 \approx 1.9635 \times 10^{-5} \text{ m}^2

Next, we find the mass per unit length μ\mu:

μ=density×A=1150×1.9635×1050.0226 kg/m\mu = \text{density} \times A = 1150 \times 1.9635 \times 10^{-5} \approx 0.0226 \text{ kg/m}

Using the tension TT computed earlier (for example, from m=1.20m = 1.20 kg, T=11.772 NT = 11.772 \text{ N}) and the frequency corresponding to this mass, f=170 Hzf = 170 \text{ Hz}, we can substitute in to find ll:

170=12l11.7720.0226170 = \frac{1}{2l} \sqrt{\frac{11.772}{0.0226}}

Rearranging gives:

l=120.022611.772l = \frac{1}{2} \frac{\sqrt{0.0226}}{\sqrt{11.772}}

Calculating this yields:

l0.067 ml \approx 0.067 \text{ m}

Step 3

Explain how the actual frequencies produced would be different from those that the student predicts.

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Answer

When predicting frequencies for tensions that are significantly larger than those used in the original experiment, it is important to consider the effect of increased tension on the behavior of the nylon string. As tension increases, it can have a couple of notable effects:

  1. Non-Linearity: The predictions based on the linear relationship fTf \propto \sqrt{T} assume that the string behaves linearly, which may not hold true at higher tensions.

  2. Material Properties: The nylon string could experience changes in elasticity or tension distribution at much higher tensions, which can affect frequency.

  3. Damping Effects: At higher frequencies and tensions, energy losses due to damping can be increased, further reducing the actual observed frequency compared to theoretical predictions.

Consequently, the actual frequencies observed at higher tensions may be lower than those predicted by the model, making the predictions less valid.

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