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Electric fields
for 14-16
Just as the effects of magnets and of gravity can be explained in terms of fields, the way that electric charges and circuits behave can too. Force fields provide an alternative explanation to action-at-a-distance between charged articles.
Demonstration
Comparisons with magnetic fields may be helpful here.
Apparatus and Materials
- Power supply, EHT (0-5kV) and/or Van de Graaff generator
- Polystyrene balls, metallised, approx 3 cm diameter
- Perspex rods, to hold balls, 2
- Retort stands and bosses, 2
- Perspex rod (about 60 cm) with paper vane
- Metal plates with insulating handles
Health & Safety and Technical Notes
Read our standard health & safety guidance
Paint the polystyrene balls with Aquadag or other conducting paint, or spray them with antistatic spray to give them a conducting surface. (Metal balls are equally good, but they should be large: diameter at least 5 cm.) Support each on a horizontal insulating rod (e.g. Perspex). Tape a small piece of aluminium foil onto each ball, to serve as an electrode. Use crocodile clips to attach leads to the supply.
Make a small paper vane, like a compass needle, about 4 cm long. Attach it to a long Perspex rod with a pin as pivot. The paper must be slightly conducting; paper is hygroscopic enough to ensure conduction in most cases. If necessary, breathe on the paper.
Procedure
- Fix the two balls approx 10 cm apart, centre to centre. Connect the balls through the 50 MΩ. safety resistor to the 5,000-volt supply's + and - terminals, both unearthed.
- Make sure the paper vane is free to rotate. Hold it by the long rod in the space between the balls. It will set along the field lines, because it develops induced charges in the field - rather like the behaviour of iron filings or soft iron in a magnetic field.
- Starting with the vane near one ball, move it, steering
straight ahead by the compass
to map a line of force of the electric field. Show several such lines in quick succession. Ask students where they have seen a magnetic field of similar shape. - The device can also be used to show that the lines are not straight at the edge of a plate.
Teaching Notes
- The paper indicator acts by developing induced charges in the field. This is why it must conduct, although it need not conduct well. The charges were in the paper before, in equal amounts of positive and negative charge. They cancelled out each other's effects until the field dragged them apart, so that negative charges collect at one end and positive charges at the other. The field tugs on the charged ends of the paper indicator and pulls it round until it points along the field. In this way we can map the electric field in a similar way to mapping a magnetic field with iron filings.
- With a Van de Graaff generator you may be able to show the same field patterns, but corona discharge (from the higher potential) may mar it.
This experiment was safety-tested in December 2006
Up next
Forces in an electrostatic field
Demonstration
A shuttling ping-pong ball serves as a model of ions moving in an electric field.
Apparatus and Materials
- Power supply, EHT, 0–5 kV
- Metal plates with insulating handles, 2
- Table-tennis (ping-pong) ball, coated with Aquadag
- Nylon thread, e.g. fishing line, 1 reel
- Clamp
- Retort stands and bosses, 3
Health & Safety and Technical Notes
Read our standard health & safety guidance
Although educational EHT supplies are limited to safe output currents, the shock obtained by touching the live
plate in this demonstration can make the demonstrator jump. Switch the supply off before making adjustments.
Procedure
- Attach the two metal plates to retort stands using bosses, and set them up parallel to each other 10 cm apart.
- Connect the plates directly to the positive and negative terminals of the EHT power supply using crocodile clips attached to the special lugs on the back of the plates.
- Suspend the table tennis-ball, coated with Aquadag, by nylon thread from a further retort stand so that it hangs freely between the two plates.
- Apply a potential difference of 3,000 to 4,000 volts to the plates. The ball is charged by contact with one of the plates. It will then move rapidly backwards and forwards between the two plates.
- Vary the potential difference and the separation of the plates.
Teaching Notes
- This demonstration shows the forces on a charged object in an electric field. It also serves as a model of an ion moving in an electric field. As the ball moves to and fro between the plates, it represents a positive ion moving one way and then a negative ion moving the other.
- The electric field between parallel charged plates, E = V/d, where V is the potential difference between the plates and d is the separation of the plates.
This experiment was safety-tested in June 2007
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A model of Millikan’s experiment
A model of Millikan’s experiment
Practical Activity for 14-16
Demonstration
A qualitative experiment to show the principle of a force on a charged body between two parallel plates.
Apparatus and Materials
- Macro-Millikan apparatus
- Power supply, 0–5 kV (Extra High Tension, EHT)
- Proof plane
- Polythene tile
- Charging cloth
Health & Safety and Technical Notes
Use an EHT supply of no more than 5 kV, which is current-limited to less than 5 mA.. The power supply for the heater MUST have adequate insulation. Leads used MUST have shrouded connectors and insulation capable of withstanding 5 kV.
Make all connections with the power supply turned off. Do not adjust connections while the EHT is switched on.
Electron beam tubes are fragile. Because they are evacuated, they will implode if they break. The tubes are also expensive, so handle them with great care. Use the purpose-designed holders during practical work.
Note that when switching the EHT supply off, it can take a little while for the voltage output from the EHT to fall to zero. Allow sufficient time before disconnecting.
Be Careful not to touch the exposed plates.
Read our standard health & safety guidance
The illustrations show the ‘macro-Millikan’ apparatus. It consists of a pair of metal plates, one of which has a central hole through which a small polystyrene ball can pass. The ball has a length of nylon thread attached, and at the other end of the thread is a Pyrex glass spring.
The best arrangement for securing the upper end of the spring is to attach it to another loop in a nylon thread. This is taken up over a pulley connected to the ceiling, and then to an eyelet on a block of wood. Alternatively, a support from a long retort stand rod can be used, as shown below, and brought up over the plates, forming a hooked support.
Procedure
- With the EHT switched off, set the plates up horizontally, 7 to 10 cm apart, one above the other.
- Connect the earth terminal of the power supply to its negative terminal. Connect the lower plate to the earth terminal of the EHT power supply. Connect the upper plate to the positive terminal. To reverse the field, change the leads to the supply, but in each case the lower plate should be earthed.
- Lower the small conducting sphere with its nylon suspension through the hole in the upper plate. The upper end of the nylon suspension is looped and connected to the Pyrex glass spring.
- Rub the polythene tile and put the proof plane on it, touching to charge the proof plane by induction. Without making contact with the plates, bring the proof plane up to the conducting sphere to charge it by contact. Adjust the suspension so that the sphere is almost exactly half-way between the two plates. This is most conveniently done in the first arrangement described above. By moving the block of wood nearer to or away from the apparatus, the sphere can be lowered or raised.
- Switch on the EHT supply, set at 2 - 4 kV. The sphere will move as the extra force stretches the spring. The sphere can be brought back to the central position by moving the block of wood. Students will see the movement quite clearly if their eyes are in line with the plates.
Teaching Notes
- There are no measurements to be made in this demonstration: it is a qualitative experiment to show the principle of a force on a charged body between two parallel plates. Quantitative experiments do not lead to very satisfactory results unless considerable trouble is taken. There is a tendency for the charge to leak away along the suspension.
- If the ball is near one plate, the charge on it induces an opposite charge on that plate, so there is attraction. You do not want that ‘image-force’ to appear in the demonstration. The ball must be almost exactly half-way between the two plates, so that the image forces cancel out.
- Students' eyes need to be in line with the plates. It is easier to see the movement of the ball if a plane mirror is placed behind the suspension with a horizontal line ruled across it, whilst a small cardboard disc is attached to the nylon suspension to act as a pointer. This pointer is aligned with the mark on the mirror before the field is switched on, but after the sphere has been positioned at the centre of the plate. However, this special arrangement may divert attention from the general idea and need not be used in this qualitative demonstration.
- You may like to experiment with a realistic model of the Millikan experiment. Place a very light metal-coated ball in the field between the plates. Adjust the field to make the ball float upwards, fall slowly downwards, or even remain poised at rest for a short time. The ball is charged by contact with one of the plates, which then repels it. A very light ball is needed, or perhaps a scrap of aluminium leaf. When the ball is poised, its equilibrium is made unstable by image forces. To minimize that disadvantage, the charge on the ball should be made as small as possible and the electric field as large as possible.
This experiment was safety-tested in March 2008
Up next
Electric charge and current - a short history
Electrical phenomena result from a fundamental property of matter: electric charge. The atoms that constitute most matter we encounter contain charged particles. Protons and electrons each have one unit charge, but of opposite sign. Atoms are generally neutral because the number of electrons and protons are the same.
Electric charges at rest have been known much longer than electric currents.
The amber effect
The property now called static electricity
was known to the philosophers of ancient Greece. In fact the word electricity comes from ‘elektron’, the Greek name for amber. Amber is a resinous mineral used to make jewellery. It is probable that small fibres of clothing clung to amber jewels and were quite difficult to remove. Trying to rub the fibres off made the situation worse, causing early philosophers to wonder why.
William Gilbert mentioned the amber effect
in his ground-breaking book On Magnetism, published in 1600. He noticed that the attraction between electrics
was much weaker than magnetism and wrongly said that electrics never repelled.
Benjamin Franklin
A giant leap of understanding was required to explain observations like these in terms of positive and negative electrical charge. In the 18th century, Benjamin Franklin in America tried experiments with charges. It was Franklin who named the two kinds of electricity ‘positive’ and ‘negative’. He even collected electric charges from thunderstorm clouds through wet string from a kite.
Franklin was an advocate of a ‘single fluid’ model of electric charge. An object with an excess of fluid would have one charge; an object with a deficit of fluid would have the opposite charge. Other scientists had advocated a ‘two fluid’ theory, with separate positive and negative fluids moving around. It took over a century for the debate to come down on Franklin’s side.
It is interesting to note that Franklin coined several electrical terms which we still use today: battery, charge, conductor, plus, minus, positively, negatively, condenser (= capacitor), among others.
Electric currents
Electric currents were not fully investigated until batteries were invented in about 1800. Passing currents through salt solutions provides evidence that there are two kinds of charge carriers, positive and negative. The charge carriers that boil out of white hot metals are negative electrons, and movements of electrons produce current in a cool, metal wire.
For a time electric currents seemed so different from electric charges at rest that the two were studied separately. It seemed as if there were four kinds of electricity: positive and negative electrostatic charges, and positive and negative moving charges in currents. Now scientists know better. There are just two kinds, positive and negative, exerting the same kind of forces whether they were ‘electrostatic charges from friction’ or ‘moving charges from power supplies’.
A modern view
Electric forces are what hold together atoms and molecules, solids and liquids. In collisions between objects, electric forces push things apart.
Today we understand that electrons may be transferred when two different materials contact each other and then separate. You can list materials in order, from those “most likely to lose electrons” (gaining positive charge) to "those most likely to gain electrons” (gaining negative charge). This is called the triboelectric series
.
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Electric fields
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Classroom management in semi-darkness
There are some experiments which must be done in semi-darkness, for example, optics experiments and ripple tanks. You need to plan carefully for such lessons. Ensure that students are clear about what they need to do during such activities and they are not given unnecessary time. Keep an eye on what is going on in the class, and act quickly to dampen down any inappropriate behaviour before it gets out of hand.
Shadows on the ceiling will reveal movements that are not in your direct line of sight.