Electron microscopes use a high-precision electron velocity selector consisting of an electric field, \(E\), perpendicular to a magnetic field, \(B\).
Electrons travelling at the required velocity, \(v_0\), exit the aperture at point \(\text{Y}\), while electrons travelling slower or faster than the required velocity, \(v_0\), hit the aperture plate, as shown in Figure 2.
- Show that the velocity of an electron that travels straight through the aperture to point \(\text{Y}\) is given by \( v_{0} \) = \( \dfrac{E}{B}\). (1 mark)
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- Calculate the magnitude of the velocity, \(v_0\), of an electron that travels straight through the aperture to point \(\text{Y}\) if \(E\) = 500 kV m\(^{-1}\) and \(B\) = 0.25 T. Show your working. (2 marks)
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- i. At which of the points – \(\text{X, Y}\), or \(\text{Z}\) – in Figure 2 could electrons travelling faster than \(v_0\) arrive? (1 mark)
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- ii. Explain your answer to part c.i. (2 marks)
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