Required Practical: Investigating Stationary Waves (AQA A Level Physics): Revision Note

Exam code: 7408

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Reviewed by: Timothy Sit

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Required practical: investigating stationary waves

Aims of the experiment

  • The overall aim of the experiment is to measure how the frequency of the first harmonic is affected by changing one of the following variables:

    • the length of the string

    • the tension in the string

    • strings with different values of mass per unit length

Variables:

  • Independent variable = either length, tension, or mass per unit length

  • Dependent variable = frequency of the first harmonic

  • Control variables:

    • If length is varied = same masses attached (tension), same string (mass per unit length)

    • If tension is varied = same length of the string, same string (mass per unit length)

    • If mass per unit length is varied = same masses attached (tension), same length of the string

Equipment list

Apparatus

Purpose

Signal generator

Used to operate the vibration generator and measure the frequency of the first harmonic

Vibration generator

Connected to the signal generator to produce the stationary wave

Retort stand

To provide a stable fixed end on the table

G clamp or 2 kg mass

To place on the retort stand to stabilise apparatus

2.0 m of string

Used to observe the stationary wave

Pulley

To allow the masses to hang vertically, and introduces less friction than the edge of the table

Wooden bridge

To provide the other fixed end which can vary the length of the string

Mass hanger + 100 g masses

To hang from the pulley to vary tension in the string

Metre ruler

To measure the length of the string

Top-pan balance

To measure the mass of the string

  • Resolution of measuring equipment:

    • Metre ruler = 1 mm

    • Signal generator ~ 10 nHz

    • Top-pan balance = 0.005 g

Method

  • This method is an example of the procedure for varying the length of the string with the frequency – this is just one possible relationship that can be tested

Apparatus for investigating stationary waves. A signal-generator-connected vibration generator drives a string of length L over a bridge and pulley to hanging masses. The retort stand supports the setup; tension is T equals m g.
Changing the length, tension or mass per unit length of the string changes the frequency of the first harmonic
  1. Set up the apparatus by attaching one end of the string to the vibration generator and pass the other end over the bench pulley and attach the mass hanger.

  2. Adjust the position of the bridge so that the length L is measured from the vibration generator to the bridge using a metre ruler.

  3. Turn on the signal generator to set the string oscillating.

  4. Increase the frequency of the vibration generator until the first harmonic is observed and read the frequency that this occurs at.

  5. Repeat the procedure with different lengths.

  6. Repeat the frequency readings at least two more times and take the average of these measurements.

  7. Measure the tension in the string using T = mg

    • where m is the amount of mass attached to the string and g is the gravitational field strength on Earth (9.81 N kg–1)

  8. Measure the mass per unit length of the string μ = mass of stringlength of string.

    • Simply take a known length of the string (1 m is ideal) and measure its mass on a balance

  • An example of a table with some possible string lengths might look like this:

L / m

f / Hz
1st reading

f / Hz
2nd reading

f / Hz
3rd reading

f / Hz
Mean

0.2

0.4

0.6

0.8

1.0

1.2

1.4

1.6

Analysing the results

  • For the first harmonic, wavelength, λ = 2L

  • So, the speed of the stationary wave is:

v = fλ = f × 2L

  • Rearranging for frequency, f:

f = v2L = v2(1L)

  • Comparing this to the equation of a straight line: y = mx

    • y = f (Hz)

    • x = 1L (m−1)

    • Gradient = v2 (m s−1)

  1. Plot a graph of the mean values of f against 1L.

  2. Draw a line of best fit and calculate the gradient.

  3. Work out the wave speed, which will be 2 × gradient:

A straight-line graph of frequency against 1/L passing through the origin. It is labelled “gradient = fL” and “v = 2 × gradient”.
If the frequency is plotted against the inverse of the length, the velocity is twice the gradient of the graph
  • Verify the wave speed of the travelling waves using the equation:

v = Tμ

  • Where:

    • T = tension (N)

    • μ = mass per unit length (kg m−1)

  • Assess the uncertainties in the measurements of length and the frequency and carry out calculations to determine the uncertainty in the wave speed

Evaluating the experiment

  • Systematic errors:

    • An oscilloscope can be used to verify the signal generator’s readings

    • The signal generator should be left for about 20 minutes to stabilise

    • The measurements would have a greater resolution if the length used is as large as possible, or as many half-wavelengths as possible

      • This means measurements should span a suitable range, for example, 20 cm intervals over at least 1.0 m

  • Random errors:

    • The sharpness of resonance leads to the biggest problem in deciding when the first harmonic is achieved

      • This can be resolved by adjusting the frequency while looking closely at a node — this is a technique to gain the largest response

      • Looking at the amplitude is likely to be less reliable since the wave will be moving very fast

    • When taking repeat measurements of the frequency, the best procedure is as follows:

      • Determine the frequency of the first harmonic when the largest vibration is observed and note down the frequency at this point

      • Increase the frequency and then gradually reduce it until the first harmonic is observed again and note down the frequency of this

      • If taking three repeat readings, repeat this procedure again

      • Average the three readings and move onto the next measurement

Safety considerations

  • Use a rubber string instead of a metal wire, in case it snaps under tension

  • If using a metal wire, wear goggles to protect the eyes in case it snaps

  • Stand well away from the masses in case they fall onto the floor

  • Place a crash mat or any soft surface under the masses to break their fall

Worked Example

A student investigates the relationship between the frequency of the stationary waves on a wire and the tension in the wire. The tension is varied by adding masses to a hanger which is attached to a pulley over one end of a table. The student records the following data:

  • Mass of the wire = 0.16 g

  • Length of the wire weighed = 1.0 m

  • Distance between the fixed ends = 0.4 m

Mass on hanger / kg

Frequency / Hz

1st reading

Frequency / Hz

2nd reading

Frequency / Hz

Mean

0.20

140

135

0.40

195

200

0.60

240

240

0.80

280

278

1.00

310

310

1.20

340

340

1.40

365

368

1.60

392

390

Calculate the frequency using the relation between frequency, length, tension and mass per unit length. Evaluate the percentage uncertainty in these values.

[7]

Answer:

Step 1: Calculate the mean values of frequency

  • The mean readings are: 138 Hz; 198 Hz; 240 Hz; 279 Hz; 310 Hz; 340 Hz; 367 Hz; 391 Hz

Step 2: Work out the tensions and mass per unit length

  • Use the equation to calculate the frequency for a mass of 0.20 kg:

μ = 0.16 × 10−31.0 = 0.16 kg m−1 [1 mark]

T = mg = 0.20 × 9.81 = 1.96 N

f = 12LTμ = 12 × 0.4 × 1.960.16 × 10−3 [1 mark]

f = 138.3 = 140 Hz (2 s.f.)

  • Working in the same way, the frequencies for the remaining lengths are: 200 Hz; 240 Hz; 280 Hz; 310 Hz; 340 Hz; 370 Hz; 390 Hz [1 mark]

Step 3: Determine the uncertainties in each quantity

  • Mass on hanger

    • The maximum uncertainty is likely to be 0.005 kg

    • Therefore, % uncertainty in measurement of 0.2 kg is 0.0050.20 × 100% = 2.5%

    • Since each mass has an uncertainty of 0.005 kg, these are added together as the masses increase, so each mass has the same percentage uncertainty i.e. 0.010.40 × 100% = 2.5% [1 mark]

  • Length

    • Resolution of a metre ruler is 1 mm, but errors of up to 1 cm are possible in this set up

    • Therefore, % uncertainty in measurement of 0.4 m is 0.010.4 × 100% = 2.5% [1 mark]

  • Mass per unit length

    • The resolution of a metre ruler is 1 mm and the resolution of a top-pan balance is 0.005 g

    • Therefore the uncertainty in the mass per unit length:

      • ∆μμ = ∆mm + ∆ll

      • ∆μ = 0.16 × (0.0050.16 + 0.0011.0) = 0.005 g m−1

    • Therefore, % uncertainty in measurement of 0.16 g m-1 is 0.0050.16 × 100% = 3% [1 mark]

Step 4: Determine the uncertainties in the mean frequency values

  • Since tension (proportional to the mass on the hanger) and mass per unit length are to the power of 12, their % uncertainties are halved

  • Maximum % uncertainty in calculated frequencies would be the % uncertainty in each value added together:

    • % uncertainty in frequency = 2.5% + 1.25% + 1.5% = 5.25% [1 mark]

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Katie M

Author: Katie M

Expertise: Curriculum Expert

Katie has always been passionate about the sciences, and completed a degree in Astrophysics at Sheffield University. She decided that she wanted to inspire other young people, so moved to Bristol to complete a PGCE in Secondary Science. She particularly loves creating fun and absorbing materials to help students achieve their exam potential.

Timothy Sit

Reviewer: Timothy Sit

Expertise: Content Creator

Timothy graduated with a first class degree in Mathematics and Physics from the University of Warwick. After working as a postgraduate researcher, Timothy has worked as a content creator for various online revision platforms, creating physics resources for a range of levels and exam boards.