Tag Archive for: core

Simple harmonic motion

A-Level Physics Required Practicals:
Simple Harmonic Motion

(and a bit of error analysis)

Supporting notes for this film will follow shortly.

Assessment

— to follow

Student Worksheet

— to follow

Comments & Feedback

As ever, no single film can encompass everything one might wish to say about a practical. Please, leave comments with your thoughts about the approach we’ve taken, and your suggestions for alternatives or improvements.


Inverse Square Law

A-Level Physics Required Practicals:
Inverse Square Law

Supporting notes for this film will follow shortly.

Assessment

— to follow

Student Worksheet

— to follow

Comments & Feedback

As ever, no single film can encompass everything one might wish to say about a practical. Please, leave comments with your thoughts about the approach we’ve taken, and your suggestions for alternatives or improvements.


Force on a Current-Carrying Wire

A-Level Physics Required Practicals:
Force on a Current-Carrying Wire

Supporting notes for this film will follow shortly.

Assessment

— to follow

Student Worksheet

— to follow

Comments & Feedback

As ever, no single film can encompass everything one might wish to say about a practical. Please, leave comments with your thoughts about the approach we’ve taken, and your suggestions for alternatives or improvements.


Diffraction

A-Level Physics Required Practicals:
Investigating Diffraction Using a Laser

All the new specifications include a required practical that asks students to measure the wavelength of light by diffraction. Some awarding bodies insist on the use of a laser, while others allow alternative light sources. Some expect the use of Young’s double slits, whilst others suggest a diffraction grating.

In both cases, the light diffracts as it passes through the slits, leading to a broader spread of light on a screen. The different beams diffracted by each slit interfere with each other, either constructively or destructively, depending on their relative path length between slit and screen.

This is a great opportunity to carry out careful measurements, to revise geometry and trigonometry, and to discuss the nature of light itself.

In this film, we show first the double slit method set up conventionally, and then a method using a diffraction grating arranged vertically. Both approaches use laser pointers. The vertical arrangement has advantages in terms of both space in the lab and experiment safety, which are covered in the film.

Using lasers

Many teachers are – quite rightly – concerned about the safety implications of using multiple lasers in a class, even with reasonably sensible students. Particular concerns include:

  • With multiple sets of apparatus it can be hard to avoid having laser beams (or their reflections or diffraction paths) criss-crossing the lab.
  • In many labs it’s hard to achieve a good blackout, and that carries its own classroom management issues: do you have appropriate places to store coats and bags, for example? What about trailing cables and other trip hazards, in a darkened environment?
  • Lasers can be sourced for very little money, but they’re often more powerful than the claimed “<1 mW”. Christina started what turned out to be an interesting discussion about how one might check this, on Talk Physics (registration required).

As ever, one should check with CLEAPSS. Here’s their guidance on lasers (PDF link). Their recommendation is to purchase from an established office or IT supplier, and to ensure the specific unit you receive has a CE marking and a classification BS EN 60825 Class 2. But that’s a summary: read the CLEAPSS advice in full.

It is possible to avoid lasers by using a white light source with a coloured filter. However, to get good results the source needs to be very bright, ideally narrow (collimated), and as close to monochromatic as possible. In practice the filter often costs more than a suitable laser, but if you’d like to explore the option, here’s a write-up at Practical Physics.

Young’s Double Slits

As shown in the film, different exam boards and textbooks use different notation for the formula governing the diffraction of light using a double slit aperture:

\(\lambda = ax / D\)

where:

  • \(\lambda\) = wavelength of light (to be found)
  • \(a\) = slit spacing, between centres – this information is probably printed on a double-slit slide.
  • \(x\) = fringe separation, between adjacent maxima or minima. Measure with a ruler or Vernier callipers, or use mm squares on graph paper as the screen.
  • \(D\) = distance from slits to screen, which should be as large as possible (ideally 2 m or more).

Alternatively:

\(\lambda = ws/D\)

where:

  • \(s\) = slit spacing
  • \(w\) = fringe separation

A straightforward calculation can be done, or you can use the graphical method Alom describes in the film at 1’04”, plotting the fringe separation obtained for a range of different \(D\) values and using the gradient to calculate \(\lambda\). You can check the value you obtain against the value stated on the laser and see if it agrees, within your experimental uncertainty.

Questions you might ask your students:

  • Why is a laser a particularly suitable light source for this experiment?
  • What would happen to the fringe spacing if we used a green or blue laser? Why?
  • Why do we want \(a\) (or \(s\)) to be as small as possible, and \(D\) as large as possible?
  • What are the uncertainties in the measured quantities, and how do we combine those to arrive at an uncertainty in \(\lambda\)?

Diagram

We have a PDF version of the above diagram available for download.

Diffraction Grating

This is an alternative or additional method. The pattern obtained is easier to see, since the bright fringes (maxima) are well-defined ‘spots’. however, the mathematics involved is a little more involved, and students must use trigonometry to find the diffraction angle \(\theta\).

In the film, Christina sets up the apparatus vertically, which both requires less space in the lab and reduces concerns over laser safety. However, you will still need to be cautious for stray reflections.

The relationship here is

\(n\lambda = d \sin\theta\)

where:

  • \(n\) = the order of the maximum, with \(n=0\) as the central maximum, \(n=1\) for the ‘first order’ to either side, and so on.
  • \(\lambda\) = wavelength of light
  • \(d\) = slit spacing. Usually a diffraction grating slide states the number of lines per mm. For example: 300 lines/mm implies 300,000 slits/m, so \(d = 1/300,000~\mathrm{m}\).
  • \(\theta\) = angle between the straight-through direction (helpfully marked by the zero-order maximum) and the maximum being investigated. This must be found using trigonometry:

As stated in the film (at 3’15”), we cannot use the small angle approximation here, since the angles are too large. Hence:

\(\theta = \tan^{-1}(\frac{x}{D})\)

Using the measurements in the film, Alom’s miraculous ‘off-the-cuff’ calculation went like this:

  • Total distance = 191 mm, so \(x\) = 191/2.
  • \(D\) = 225 mm
  • So \(\theta = \tan^{-1}((191/2)/225) = 22.9985\) ≈ 23.0°

Now, to calculate the wavelength:

\(n\lambda = d\sin\theta\) or \(\lambda = \frac{d\sin\theta}{n}\)

Since we measured two fringes either side of the central maximum (for accuracy):

  • \(n = 1\)
  • \(d = \frac{1}{300,000}~\mathrm{m}\)
  • \(\lambda = (\frac{1}{300,000}\sin 22.9985)/2 = 6.5118 \times 10^{-7} = 651~\mathrm{nm}\) (to 3 sf).

Again, students can compare this with the manufacturer’s stated value; the students should be able to assess their uncertainty to check that the manufacturer’s value falls within their uncertainty range. The same discussions as above can be had about how to minimise uncertainties, and what would happen if a different colour laser were to be used.

Further work

Christina suggests in the film that for an extension activity, students could be given an unmarked diffraction grating with a different (and unknown) slit spacing, and asked to use the laser wavelength they’ve calculated to measure the slit spacing. As set out earlier, white light could be used with a colour filter, and the comparisons of uncertainties would be interesting.

Materials & Costs

Double slit slides: can be bought for around £10 each, for example from Philip Harris.

Gratings: eg. 300 lines/mm for around £15, again from Philip Harris.

Assessment

Common Practical Assessment Criteria

At the time of writing, the exam boards appear to agree that this practical might be used to address CPAC 3 and 4, or subsets of them. For example, AQA suggests:

  • using appropriate analogue apparatus to record a range of measurements (to include length/distance, angle)
  • using a laser or light source to investigate characteristics of light, including interference and diffraction.

Student Worksheet

We’ve drafted a student worksheet for this practical, which you may find useful:

Comments & Feedback

As ever, no single film can encompass everything one might wish to say about a practical. Please, leave comments with your thoughts about the approach we’ve taken, and your suggestions for alternatives or improvements.


Discharging a Capacitor

A-Level Physics Required Practicals:
Investigating the Discharge of a Capacitor

All the new specifications include a required practical that asks students to investigate capacitors charging or discharging through a resistor. The awarding bodies agree that this practical is an ideal opportunity for students to develop their skills in using ICT.

What’s in the Film

It’s possible to measure the changing potential difference across the capacitor using:

  • A voltmeter and stopwatch.
  • An oscilloscope (whether cathode ray or digital, for example a Picoscope).
  • A datalogger.

The circuit will be similar whichever approach you use. A meter connected in parallel across the resistor R measures V. With the switch connected at A, the capacitor C charges (almost instantly, since there is negligible resistance in the circuit). When the switch is flicked to position B the capacitor discharges through the resistor, with both the current and voltage decreasing exponentially.

In their experiments, both Alom and Carol do without a two-way switch and instead simply disconnect the capacitor from the power supply to make it discharge through the resistor.

As Alom mentions in the introduction, the uses of capacitors are quite interesting for giving the students some context here. He refers to a previous film:


The Datalogger Method

In core practical film, Alom uses Edu-lab data loggers (see below for approximate costings), but there are many alternatives. You could also use a digital oscilloscope which stores data, or a computer-based ‘Picoscope’ or similar which functions equivalently.



From 1’32” in the film Alom suggests that students can check the discharge curve is exponential by seeing if there is a constant half-life (the time taken for the potential difference to fall by a half). Or, better, to measure the time constant and if it that is… er… constant (the time constant is the time taken for the measured potential difference to drop to 1/e of its original value – see the graph above).

Earlier in the film, Alom chooses values for and R which multiply to give a time constant which is measurable: neither too fast nor too slow. In this case:

\(C = 4700~\mathrm{\mu F}\)
\(R = 10~\mathrm{k\Omega}\)
So time constant \(\tau = 4700\times10^{-6} \cdot 10 \cdot 10^3 = 47~\mathrm{s}\)

The exponential equation:

\(V = V_{0}e^{-t/RC}\)

is one which students will need to be able to handle. Alom shows how to manipulate this into the form of a straight-line graph. First, take natural logs of both sides:

\(ln(V) = ln(V_0) – \frac{t}{RC}\)

Compare with:

\(y = mx + c\)

If \(ln(V)\) is plotted on the y-axis against \(t\) on the x-axis, then \(ln(V_0)\) will be the y-intercept and \(-\frac{1}{RC}\) the gradient, hence \(C\) if \(R\) is known.


Resistor colour code

This might be a useful opportunity to show students the resistor colour code:

Questions

You might like to ask your students:

  • Why is a datalogging method appropriate for this practical?
  • Does it matter which way round we connect the capacitor? (see Carol’s comment at 3’21).
  • For how long should we time the discharge?
  • What would happen if we instead measured V while the capacitor charges?
  • Why process the data so we get a straight line graph? Why is this better than a curve?
  • What should the units of \(ln(V)\) be?

The Direct Measurement Method

Carol uses a multimeter as a voltmeter and a stopclock to do the timing manually. She suggests measuring V every ten seconds: it’s hard to record it any more frequently, but take less frequent measurements and the graph will be hard to draw, with too few data points. Any voltmeter will do: digital, analogue, multimeter, or even an oscilloscope.

Students could be challenged to find an unknown capacitance by measuring the time constant obtained with a particular resistor. In the film, Carol explains that some preliminary runs will be needed to test the circuit and to ensure they have a suitably measurable time constant.

This method lends itself to the use of ICT, in that students can put their data into a spreadsheet and manipulate them into a straight line for (as shown above). Alternatively, data can be processed by hand.

You might as your students:

  • Why do we not need to worry about starting the timing immediately the discharge begins? (This will test their understanding of the exponential decay function.)
  • What are the causes of uncertainty in the experiment – not only our measurements, but the manufacturers’ tolerances for their components?
  • How can we reduce the uncertainty in our readings?

Safety

Since \(Q = CV\), a large capacitor charged to a huge voltage stores a lot of charge, which will lead to a high initial charging or discharging current, with consequent heating effect. The values used in the film (and noted above) offer a good guide to what works well – and safely.

Capacitors should not be charged to a voltage higher than that stated on their labelling or product information sheets. Electrolytic capacitors should be connected with the correct polarity.

It’s also important to ensure the capacitor is discharged before touching it: disconnect the power, then operate the circuit to discharge the capacitor through the resistance before dismantling the apparatus.

Costs

The Edu-logger system used in the film sells for around:

  • £45 for the voltage sensor
  • £43 for the USB module to connect to a PC (standalone display/tablet/smartphone alternatives are available).
  • £43 for a battery module.

Those figures are without VAT. Other systems are available for similar prices, or you can spend considerably more on systems with increasing levels of flexibility. Most suppliers will offer discounts on bulk orders.

Further work

The IOP’s Teaching Advanced Physics website has a series of articles about teaching topics around capacitance:

Assessment

Common Practical Assessment Criteria

At the time of writing, the exam boards appear to agree that this practical might be used to address, in whole or in part:

  • CPAC 3: Safely use a range of practical equipment and materials.
  • CPAC 4: Makes and records observations.

Student Worksheet

We’ve drafted a student worksheet for this practical, which you may find useful as a starting point:

Comments & Feedback

As ever, no single film can encompass everything one might wish to say about a practical. Please, leave comments with your thoughts about the approach we’ve taken, and your suggestions for alternatives or improvements.