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In an experiment the tension of a vibration string was kept constant while its length was varied so as to tune the string to series of vibrating tuning forks. A student obtained the following result: Draw a graph for the set of observation and fit the "best" straight line to them.

Physics

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3 parts
b

21160 Hz⋅cm\text{21160 Hz}\cdot\text{cm}

-16.6 Hz\text{-16.6 Hz}

c

f=21160L−16.6f = \frac{21160}{L} - 16.6

d

453.6 Hz\text{453.6 Hz}

Step-by-step solution

8 steps

The relationship between the frequency (ff) and length (LL) of a vibrating string with constant tension is given by f=12LTμf = \frac{1}{2L} \sqrt{\frac{T}{\mu}}, where TT is tension and μ\mu is linear density. This implies that ff is inversely proportional to LL, or f∝1Lf \propto \frac{1}{L}. To obtain a straight line graph, we should plot ff against 1L\frac{1}{L}.

First, let's calculate 1L\frac{1}{L} for each data point.

Frequency ff (Hz)Length LL (cm)1L\frac{1}{L} (cm⁻¹)f⋅Lf \cdot L (Hz·cm)
24678.10.0128019212.6
28869.80.0143320102.4
32062.50.0160020000.0
38452.10.0191919998.4
31239.20.0255112230.4

Notice that the product f⋅Lf \cdot L is approximately constant for the first four points (around 20000 Hz·cm), but the last point (312 Hz, 39.2 cm) gives a significantly different product (12230.4 Hz·cm). This indicates that the last data point is an outlier. For the "best" straight line fit, we will exclude this outlier and use the first four data points for the linear regression.

Part a· 2 steps

**Draw a graph for the set of observation and fit the "best" straight line to them.

  1. Prepare the data for plotting.

    Calculate the inverse of the length, 1L\frac{1}{L}, for each of the first four data points:

    • For L=78.1 cmL = 78.1 \text{ cm}, 1L=178.1≈0.01280 cm−1\frac{1}{L} = \frac{1}{78.1} \approx 0.01280 \text{ cm}^{-1}
    • For L=69.8 cmL = 69.8 \text{ cm}, 1L=169.8≈0.01433 cm−1\frac{1}{L} = \frac{1}{69.8} \approx 0.01433 \text{ cm}^{-1}
    • For L=62.5 cmL = 62.5 \text{ cm}, 1L=162.5=0.01600 cm−1\frac{1}{L} = \frac{1}{62.5} = 0.01600 \text{ cm}^{-1}
    • For L=52.1 cmL = 52.1 \text{ cm}, 1L=152.1≈0.01919 cm−1\frac{1}{L} = \frac{1}{52.1} \approx 0.01919 \text{ cm}^{-1}
  2. Describe how to draw the graph.

    Plot frequency ff (in Hz) on the y-axis and 1L\frac{1}{L} (in cm⁻¹) on the x-axis. Mark the four data points: (0.01280,246)(0.01280, 246), (0.01433,288)(0.01433, 288), (0.01600,320)(0.01600, 320), and (0.01919,384)(0.01919, 384). Draw a straight line that best fits these four points. This line should pass close to the origin, as theoretically, f=0f=0 when L→∞L \to \infty (i.e., 1L=0\frac{1}{L}=0).

Part b

21160 Hz⋅cm\text{21160 Hz}\cdot\text{cm}

**Find the slope and intercept of the graph.

  1. Calculate sums for linear regression using the first four points.

    Let x=1Lx = \frac{1}{L} and y=fy = f.
    n=4n = 4
    ∑x=0.01280+0.01433+0.01600+0.01919=0.06232\sum x = 0.01280 + 0.01433 + 0.01600 + 0.01919 = 0.06232
    ∑y=246+288+320+384=1238\sum y = 246 + 288 + 320 + 384 = 1238
    ∑x2=(0.01280)2+(0.01433)2+(0.01600)2+(0.01919)2=0.000993445\sum x^2 = (0.01280)^2 + (0.01433)^2 + (0.01600)^2 + (0.01919)^2 = 0.000993445
    ∑xy=(0.01280×246)+(0.01433×288)+(0.01600×320)+(0.01919×384)=19.766\sum xy = (0.01280 \times 246) + (0.01433 \times 288) + (0.01600 \times 320) + (0.01919 \times 384) = 19.766

  2. Calculate the slope (mm) and intercept (cc).

    The formulas for linear regression are:

    m=n(∑xy)−(∑x)(∑y)n(∑x2)−(∑x)2m = \frac{n(\sum xy) - (\sum x)(\sum y)}{n(\sum x^2) - (\sum x)^2} c=(∑y)(∑x2)−(∑x)(∑xy)n(∑x2)−(∑x)2c = \frac{(\sum y)(\sum x^2) - (\sum x)(\sum xy)}{n(\sum x^2) - (\sum x)^2}

    Substitute the calculated sums:

    m=4(19.766)−(0.06232)(1238)4(0.000993445)−(0.06232)2m = \frac{4(19.766) - (0.06232)(1238)}{4(0.000993445) - (0.06232)^2} m=79.064−77.159360.00397378−0.0038837824m = \frac{79.064 - 77.15936}{0.00397378 - 0.0038837824} m=1.904640.00009000≈21162.67 Hz⋅cmm = \frac{1.90464}{0.00009000} \approx 21162.67 \text{ Hz} \cdot \text{cm}

    Rounding to four significant figures, the slope is 21160 Hz⋅cm\boxed{\text{21160 Hz}\cdot\text{cm}}.

    c=(1238)(0.000993445)−(0.06232)(19.766)0.00009000c = \frac{(1238)(0.000993445) - (0.06232)(19.766)}{0.00009000} c=1.22949011−1.230980120.00009000c = \frac{1.22949011 - 1.23098012}{0.00009000} c=−0.001490010.00009000≈−16.555 Hzc = \frac{-0.00149001}{0.00009000} \approx -16.555 \text{ Hz}

    Rounding to three significant figures, the intercept is -16.6 Hz\boxed{\text{-16.6 Hz}}.

Part c

f=21160L−16.6f = \frac{21160}{L} - 16.6

**Find the relationship between the frequency (f) of the vibration and the length (l) of the stretched string.

  1. State the theoretical relationship.

    The theoretical relationship for a vibrating string is f=k⋅1Lf = k \cdot \frac{1}{L}, where kk is a constant.

  2. State the experimental relationship.

    Using the calculated slope (mm) and intercept (cc) from part (b), the experimental relationship is in the form f=m(1L)+cf = m \left(\frac{1}{L}\right) + c.
    Substituting the values:

    f=21160(1L)−16.6f = 21160 \left(\frac{1}{L}\right) - 16.6

    The relationship is f=21160L−16.6\boxed{f = \frac{21160}{L} - 16.6}, where ff is in Hz and LL is in cm.

Part d

453.6 Hz\text{453.6 Hz}

**What is the frequency of an unmarked fork which was in tune with a length of 45.0 cm?

  1. Use the relationship found in part (c).

    Given L=45.0 cmL = 45.0 \text{ cm}.

    f=21160L−16.6f = \frac{21160}{L} - 16.6
  2. Substitute the value of LL and calculate ff.

    f=2116045.0−16.6f = \frac{21160}{45.0} - 16.6 f=470.222...−16.6f = 470.222... - 16.6 f=453.622... Hzf = 453.622... \text{ Hz}

    Rounding to one decimal place, the frequency is 453.6 Hz\boxed{\text{453.6 Hz}}.

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