TAP 413-2: Measuring the charge to mass ratio for an electron

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TAP 413-: Measuring the charge to ass ratio for an electron Using circular otion Using a agnetic field to drive an electron round in a circle can give inforation about the acceleration. The agnetic force acting is F = qvb and the force required to drive it round in a circle is given by v F =. r You can put these two equal to get q = v. rb So three easureents can give the charge / ass ratio of the electron. Both the radius of the circular otion and the agnetic field strength can be easured in a fairly straightforward way. The easureent of the velocity, however, is harder. Electrons are accelerated by an electron gun. So Vq = 1 v so at first sight it looks as if you need q and to get started. However, aths coes to our aid, allowing you to cobine the two sets of relationships to get q = V r B (arrange both relationships to give v then put the equal). Now we can easure three things in the laboratory in order to find the charge to ass ratio for the electron. By extension you easure the charge / ass ratio for any charged particle, allowing you to characterise any particles. You will need: fine bea tube stand HT, 0 150 V power supply, 5 V dc rheostat Helholtz pair of coils 4 leads with sprung shrouds for connections to HT circuits (soe ay need a feale terination)

Safety Wire carefully, no bare conductor above 40 V. HT supplies are always dangerous, especially so in the dark. Shrouded plug leads MUST be used. No connections should be changed with the power switched on. current-carrying coil electron gun 0-150 V Making the easureents You will need to arrange the agnetic field and accelerating pd so that you can see a coplete circular electron path.

Record the pd and radius of the bea (in etres). Switch off the HT. Now reove the electron tube to allow the use of a calibrated agnetic field sensor, or a current balance, to easure the agnetic field where the electron bea was. Now use the relationship q V = r B to find q/. You have 1. Seen an arrangeent of electric and agnetic fields that will drive electrons round in a circle.. Analysed the otion to give a relationship between q/ and things you can easure in the school laboratory. 3. Made a easureent of q/.

Practical advice You will need to set this deonstration up in a well darkened roo for axiu effect, ore so than that needed for a deflection tube. You will also want to think carefully about how to display both the tube, in order to explain its action, and the resulting circle, to the size of group that you will be showing it to. Try covering the back of the tube with a black cloth If new to wiring up electron deflection tubes you ay well also wish to practice beforehand, and have a sall bench top lap to hand, well shaded so as not to destroy the dark adaptation of the group s eyes. You will need to explain and show the actions of the electron gun and the coils, probably using a giballed bar agnet to show the direction of the field. Make soe play of the need to easure the agnetic field separately, using a technique failiar to the students. This is likely to involve the use of a current balance, or a calibrated agnetic field probe. A suitable design of current balance is the following: Student ingenuity can be harnessed to estiate the radius of the circle of the electron bea. With prior practice you will, in any case, have a good idea of the values you need to obtain in order to get an approxiately correct value of q/ about 1.8 x 10 11 C kg 1. You will probably get a spread of circles, perhaps due to the field being non-unifor (a Helholtz pair only produce an approxiately unifor field in the central third of the volue they enclose), due to the electrons provided by the electron gun having a range of velocities, and due to rando theral otion superiposed on the velocity acquired fro the action of the accelerating pd.

Alternative approach Wire the circuits before the deonstration so the tube is ready to switch on. The use of the current balance can be tricky. Use a calibrated Hall probe or you could NI calculate the agnetic field using the forula for Helholtz coils B 0.7μ0 where R is R the radius of the coil, N the nuber of turns and I the current in aps. You would have to include an aeter in series with the coils to easure the current during the experient. Students do not need to know the forula for Helholtz coils. Safety Wire carefully, no bare conductor above 40 V. HT supplies are always dangerous, especially so in the dark. Shrouded plug leads MUST be used. No connections should be changed with the power switched on. External reference This activity is taken fro Advancing Physics chapter 16, 160D