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1 The type of radiation counter or Geiger-Mueller tube and counter that is available in schools varies dramatically Your procedure should take into consideration how to assemble and handle the type of equipment that is available for your use both the detector and the radioactive material 2 With the detector at least 1 m away from the radioactive materials, turn on the detector and measure the radiation This is called background radiation Record your data in the data table 3 Measure the beta and gamma radiation from your sources at various distances 4 Subtract the background count rate from the count rate recorded to obtain the corrected activity 5 Be sure to check with your teacher and have your design approved before you proceed with the lab

3 Make and Use Graphs Make a plot of the corrected sample count rate versus 1/d 2 for the beta and gamma data

1 Explain how the two graphs compare What relationship exists between distance and count rate 2 Explain how the background count rate would compare if you were at sea level, such as along the coast, compared to the level in the Rocky Mountains 3 Describe what happens to the beta count rate when the Geiger-Mueller tube is moved back to three times the initial distance; for example, 18 cm as compared to 6 cm

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keypad header on the bottom will greatly simplify the stripboard circuit, as well as the connection to the master processor Testing the Breadboard Circuit When you have assembled your breadboard circuit, we re ready to discuss our first program (keypad1bas), which is presented in Listing 11-1 Its purpose is to determine how closely our realworld ADC values match the theoretical values that were presented back in Figure 11-2 The main program loop repetitively carries out the following tasks:

1 Observe and Infer What is the background radiation source in this experiment 2 Make and Use Graphs Make a plot of gamma count rate versus distance, placing distance on the horizontal axis and corrected sample count rate on the vertical axis If the count rate levels are similar, plot the beta count rate on the same graph, and label the graph for each set of data

For several decades, physicists have been seeking to create and sustain a fusion reaction that will generate more energy than it consumes A thermonuclear reactor would generate great heat from small amounts of deuterium, 2H, 1 and tritium, 3H, which can be extracted from 1 seawater To initiate a fusion reaction, a mixture of deuterium and tritium must be heated and compressed under conditions typical of those in the Sun The required temperature would destroy the sort of containers used in fission plants Confining the plasma is one of the chief design problems for fusion reactors Magnetic Confinement In a magnetic

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confinement reactor, a strong current is passed through a container of deuterium and tritium gas so that the plasma is compressed within the arc Additional magnetic fields shape the plasma stream, as shown in the diagram, confining it away from the container walls One promising configuration keeps the plasma in a toroid, or donut shape, which has the great advantage of having no ends to seal outer layer of the pellet so quickly that it explodes Simultaneously the remainder of the pellet is compressed and heated so greatly that a fusion reaction starts The energy from the fusion of the pellet exceeds the energy used to heat the pellet A stream of pellets is fused one after another to obtain a sustained reaction, and the obtained heat is captured to create steam for turbines

In inertial confinement, beams of light or X rays from a laser rapidly heat the surface of the pellet, forming a surrounding plasma envelope The rest of the fuel is compressed by the blowoff of the hot surface material

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