9702/53

Physics 9702/53May/June 2015

Cambridge A-Level · Planning, Analysis and Evaluation · worked solutions for every part, with the mark scheme

2
questions
30
marks
75
minutes

Topics Analysis, Conclusions and Evaluation · Planning

Q115MPlanningAnalysis, Conclusions and EvaluationFree sample

A student is investigating simple harmonic motion using an electric vibrator. A plate is attached to the top of the electric vibrator. A small mass is placed on the metal plate as shown in Fig. 1.1.

An alternating potential difference (p.d.) is applied to the vibrator. For a given peak p.d. VV, there is a maximum frequency ff at which the small mass remains in contact with the plate. The contact between the small mass and plate is lost when the frequency is greater than ff.

It is suggested that the relationship between ff and VV is

k=π2f2Vk = \pi^2 f^2 V

where kk is a constant.

Design a laboratory experiment to test the relationship between ff and VV. Explain how your results could be used to determine a value for kk. You should draw a diagram, on page 3, showing the arrangement of your equipment. In your account you should pay particular attention to

(a) the procedure to be followed,
(b) the measurements to be taken,
(c) the control of variables,
(d) the analysis of the data,
(e) the safety precautions to be taken.

DifficultyMedium-Hard
Worked solution

Apparatus (with diagram)

Signal generator (sine output) + power amplifier to drive vibrator, metal plate on vibrator, small metal mass, oscilloscope (or AC voltmeter) to measure peak p.d. VV across vibrator, frequency meter / read ff from generator display, clamp stand, ruler/set square to keep plate horizontal, safety screen.

Procedure

  1. Set up vibrator with plate horizontal. Place the same small mass at the same position on the plate.
  2. Set a chosen peak p.d. VV across the vibrator (measure with oscilloscope; adjust generator/amplifier until required peak value is obtained).
  3. Starting at low frequency, increase frequency slowly until the mass just begins to lose contact (first clear bouncing / momentary separation). Record this maximum frequency ff.
  4. Repeat step 3 at least 3 times for the same VV and take the mean ff.
  5. Repeat steps 2–4 for at least 6 different values of VV over a suitable range.

Measurements

For each run record:

  • peak p.d. VV (with an uncertainty from oscilloscope scale / voltmeter resolution),
  • maximum frequency ff at loss of contact (with uncertainty from frequency display / meter),
  • repeat values and mean ff.

Control of variables

  • use the same mass throughout (mass, material and shape unchanged),
  • keep plate horizontal and surface condition the same (clean/dry),
  • keep the mass at the same position on the plate,
  • keep waveform the same (sinusoidal),
  • allow vibrator to cool / keep temperature approximately constant.

Analysis (to test relationship and find kk)

Given

k=π2f2Vk = \pi^2 f^2 V

Rearrange to linear form:

f2=kπ2(1V)f^2 = \frac{k}{\pi^2}\left(\frac{1}{V}\right)
  1. Calculate f2f^2 for each reading and tabulate f2f^2 and 1/V1/V.
  2. Plot graph of f2f^2 (y-axis) against 1/V1/V (x-axis) with error bars.
  3. Determine gradient mm of best-fit line.
  4. Then
m=kπ2    k=mπ2m = \frac{k}{\pi^2}\;\Rightarrow\; k = m\pi^2

(Scatter about a straight line through the origin supports the suggested relationship.)

Safety

  • Fit a safety screen / wear eye protection in case the mass is ejected.
  • Clamp vibrator securely; keep fingers clear of the vibrating plate.
  • Use low voltage where possible; check insulation and do not overload the amplifier.

Answer

See working

Final answer

See working

Detailed explanation

Background Concept

In simple harmonic motion (SHM), the motion is sinusoidal and the acceleration is proportional to displacement. For SHM with frequency ff and angular frequency ω\omega, we have

ω=2πf\omega = 2\pi f

A key idea for a mass on a vibrating plate is the contact condition. The mass remains in contact with the plate only while the plate can provide a normal reaction force R0R \ge 0. The instant contact is just lost is typically when the plate’s downward acceleration is large enough that the required reaction would become zero. In many vibrator experiments, the “just loses contact” point corresponds to a fixed critical acceleration related to gg.

The question gives a proposed relationship:

k=π2f2Vk = \pi^2 f^2 V

Here VV is the peak applied p.d. and ff is the maximum frequency at which contact is still maintained. The task in a Paper 5 planning question is to design a method to obtain reliable pairs (V,f)(V, f) and then analyse them in a way that would confirm (or refute) the relationship and allow kk to be found.

Understanding the Question

You are told:

  • the apparatus: an electric vibrator with a plate and a small mass on top,
  • you can control the applied alternating p.d. (peak value VV) and its frequency,
  • for each chosen VV, there exists a maximum frequency ff before the mass starts to lose contact,
  • the suggested model links the measured quantities by k=π2f2Vk = \pi^2 f^2 V.

So you must:

  1. Decide what to vary (independent variable) and what to measure (dependent variable).
  2. Describe a clear criterion for “maximum frequency” (how you decide the instant contact is lost).
  3. Explain what to keep constant (controls).
  4. Present a graph/data-processing method that yields kk.
  5. State relevant safety precautions.

Approach

A good strategy is:

  • Choose VV as the independent variable (you can set it using a signal generator/amplifier and measure it with an oscilloscope).
  • For each VV, find the threshold frequency ff where contact is just lost (increase frequency slowly and identify first clear bouncing/separation).
  • Repeat readings at each VV to reduce random judgement/timing errors.
  • Linearise the equation so a straight-line graph tests the relationship and gives kk from the gradient.

Starting from

k=π2f2Vk = \pi^2 f^2 V

divide both sides by π2V\pi^2 V:

f2=kπ2(1V)f^2 = \frac{k}{\pi^2}\left(\frac{1}{V}\right)

So a plot of f2f^2 against 1/V1/V should be a straight line through the origin, with gradient k/π2k/\pi^2.

Step-by-Step Reasoning

1) Apparatus choice and why it works

You need to control and measure two electrical quantities:

  • frequency ff (from the signal generator readout or a frequency meter),
  • peak p.d. VV across the vibrator (best measured using an oscilloscope because it directly displays peak voltage and waveform shape).

You also need a way to safely observe the mass and decide when contact is lost.

A typical workable arrangement is:

Key points:

  • The signal generator sets the frequency and (via amplifier) the drive voltage.
  • The oscilloscope across the vibrator confirms you are using a sinusoidal waveform and lets you measure the peak p.d. consistently.
  • A safety screen prevents injury if the mass is thrown off.

2) Defining variables

  • Independent variable: VV (peak p.d.).
  • Dependent variable: threshold/maximum frequency ff at which the mass just remains in contact.
  • Controls (examples that matter here): mass value, mass position, plate angle (horizontal), surface condition, waveform, and temperature/heating effects.

3) Data collection method

For each chosen VV:

  1. Set VV while watching the oscilloscope trace. If the generator setting drifts with load, re-adjust until the measured peak is correct.
  2. Start at low ff (mass clearly in contact).
  3. Increase ff slowly. Near the threshold, make small increments so you do not overshoot.
  4. Identify the threshold as the first consistent sign of separation (bouncing, visible gap, audible change, or intermittent loss of steady contact). Record ff.
  5. Repeat (at least 3 times) at the same VV and average the threshold ff.
  6. Change VV and repeat for a range (at least 6 values) to give a meaningful graph.

This repetition is essential because the “just loses contact” judgement introduces random uncertainty.

4) Table and processed quantities

Because the linear form uses f2f^2 and 1/V1/V, you should include derived columns in your table:

  • ff / Hz, f2f^2 / Hz2\text{Hz}^2,
  • VV / V (peak), 1/V1/V / V1\text{V}^{-1}.

Uncertainties:

  • ΔV\Delta V from oscilloscope scale (e.g. half the smallest division converted to volts),
  • Δf\Delta f from frequency display resolution or from repeat scatter.

5) Graph and determination of kk

Using

f2=kπ2(1V)f^2 = \frac{k}{\pi^2}\left(\frac{1}{V}\right)

Plot:

  • y-axis: f2f^2
  • x-axis: 1/V1/V

If the suggested relationship is correct:

  • points lie close to a straight line,
  • line passes through the origin within uncertainty.

Gradient mm gives:

m=kπ2    k=mπ2m = \frac{k}{\pi^2} \;\Rightarrow\; k = m\pi^2

You can estimate uncertainty in kk by finding uncertainty in gradient (worst acceptable line method) and propagating it:

Δkk=Δmm\frac{\Delta k}{k} = \frac{\Delta m}{m}

6) Safety reasoning

Main hazards are mechanical and electrical:

  • The mass may be ejected: use a screen and/or goggles.
  • The vibrator can move: clamp it securely.
  • Avoid touching the plate while operating.
  • Keep voltages within safe limits; do not overload power amplifier; inspect leads.

Key Takeaways

  • In planning questions, you must clearly state what you vary, what you measure, and what you control.
  • Test a proposed relationship by rearranging it into linear form and plotting a straight-line graph.
  • Determine constants from the gradient/intercept, and take repeats plus uncertainty estimates seriously.
  • Safety marks come from specific realistic risks and precautions.

Common Mistakes

  • Using RMS voltage from a meter when the question specifies peak VV (leads to a constant factor error).
  • Not defining a clear criterion for “maximum frequency” (vague: “when it stops working”).
  • Changing more than one variable at a time (e.g. changing mass or position between readings).
  • Plotting the wrong graph (e.g. ff vs VV) and then trying to read off kk without linearisation.
  • Forgetting units in table headings (Paper 5 expects proper headings like 1/V / V11/V\ /\ \text{V}^{-1}).

Things to Be Careful About

  • Ensure the waveform is sinusoidal; distortion changes the motion and the threshold.
  • The load of the vibrator can cause the generator’s displayed voltage to differ from the actual p.d. across the vibrator, so measure VV across the vibrator directly.
  • Near the threshold, increase ff in small steps and repeat to reduce overshoot and subjective judgement error.
  • Heating can change the vibrator response; allow cooling time or take readings quickly in a consistent order.
  • When drawing the best-fit line, use a large triangle for gradient; include error bars if you are estimating gradient uncertainty.
Techniques used
identify independent, dependent and controlled variablestake repeated readings to reduce random uncertaintylinearise the suggested relationship to obtain a straight-line graphdetermine a constant from the gradient of a graphestimate and represent measurement uncertainties with error bars

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