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Worked Example 11.1 Balancing Nuclear Reactions: Alpha Emission

Worked Example 11.1 Balancing Nuclear Reactions: Alpha Emission. Polonium-208 is one of the emitters studied by Marie Curie. Write the equation for the decay of polonium-208, and identify the element formed. Analysis.

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Worked Example 11.1 Balancing Nuclear Reactions: Alpha Emission

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  1. Worked Example 11.1 Balancing Nuclear Reactions: Alpha Emission Polonium-208 is one of the emitters studied by Marie Curie. Write the equation for the decay of polonium-208, and identify the element formed. Analysis Look up the atomic number of polonium (84) in the periodic table, and write the known part of the nuclear equation, using the standard symbol for polonium-208: Then, calculate the mass number and atomic number of the product element, and write the final equation. Solution The mass number of the product is 208 – 4 = 204, and the atomic number is 84 – 2 = 82. A look at the periodic table identifies the element with atomic number 82 as lead (Pb). Check your answer by making sure that the mass numbers and atomic numbers on the two sides of the equation are balanced:

  2. Worked Example 11.2 Balancing Nuclear Reactions: Beta Emission Write a balanced nuclear equation for the decay of chromium-55. Analysis Write the known part of the nuclear equation: Then calculate the mass number and atomic number of the product element, and write the final equation. Solution The mass number of the product stays at 55, and the atomic number increases by 1, 24 + 1 = 25, so the product is manganese-55. Check your answer by making sure that the mass numbers and atomic numbers on the two sides of the equation are balanced:

  3. Worked Example 11.3 Balancing Nuclear Reactions: Electron Capture, Positron Emission Write balanced nuclear equations for the following processes: (a) Electron capture by polonium-204: (b) Positron emission from xenon-118: Analysis The key to writing nuclear equations is to make sure that the number of nucleons is the same on both sides of the equation and that the number of charges is the same. Solution • In electron capture, the mass number is unchanged and the atomic number decreases by 1, giving bismuth-204: Check your answer by making sure that the number of nucleons and the number of charges are the same on both sides of the equation: Mass number: 204 + 0 = 204 Atomic number: 84 + (–1) = 83 (b) In positron emission, the mass number is unchanged and the atomic number decreases by 1, giving iodine-118:

  4. Worked Example 11.3 Balancing Nuclear Reactions: Electron Capture, Positron Emission Continued Check! Mass number: 118 = 0 + 118 Atomic number: 54 = 1 + 53

  5. Worked Example 11.4 Nuclear Reactions: Half-Life Phosphorus-32, a radioisotope used in leukemia therapy, has a half-life of about 14 days. Approximately what percentage of a sample remains after 8 weeks? Analysis Determine how many half-lives have elapsed. For an integral number of half-lives, we can multiply the starting amount (100%) by 1/2 for each half-life that has elapsed. Solution Since one half-life of is 14 days (2 weeks), 8 weeks represents four half-lives. The fraction that remains after 8 weeks is thus

  6. Worked Example 11.5 Nuclear Reactions: Half-Life As noted in Table 11.3, iodine-131 has a half-life of about 8 days. Approximately what fraction of a sample remains after 20 days? Analysis Determine how many half-lives have elapsed. For a non-integral number (i.e., fraction) of half-lives, use the equation below to determine the fraction of radioisotope remaining. Ballpark Estimate Since the half-life of iodine-131 is 8 days, an elapsed time of 20 days is 2.5 half-lives. The fraction remaining should be between 0.25 (fraction remaining after two half-lives) and 0.125 (fraction remaining after three half-lives). Since the relationship between the number of half-lives and fraction remaining is not linear (see Figure 11.4), the fraction remaining will not be exactly halfway between these values but instead will be slightly closer to the lower fraction, say 0.17. Solution Ballpark Check The fraction remaining is close to our estimate of 0.17.

  7. Worked Example 11.6 Ionizing Radiation: Intensity versus Distance from the Source If a radiation source gives 75 units of radiation at a distance of 2.4 m, at what distance does the source give 25 units of radiation? Analysis Radiation intensity (I) decreases with the square of the distance (d) from the source according to the equation We know three of the four variables in this equation (I1, I2, and d1) and we need to find d2. Ballpark Estimate In order to decrease the radiation intensity from 75 units to 25 units (a factor of 3), the distance must increase by a factor of Thus, the distance should increase from 2.4 m to about 4 m.

  8. Worked Example 11.6 Ionizing Radiation: Intensity versus Distance from the Source Continued Solution STEP 1:Identify known information. We know three of the four variables. STEP 2:Identify answer and units. STEP 3:Identify equation. Rearrange the equation relating intensity and distance to solve for d2. STEP 4: Solve. Substitute in known values so that unwanted units cancel. Ballpark Check The calculated result is consistent with our estimate of about 4 m.

  9. Worked Example 11.7 Balancing Nuclear Reactions: Transmutation Californium-246 is formed by bombardment of uranium-238 atoms. If 4 neutrons are also formed, what particle is used for the bombardment? Analysis First write an incomplete nuclear equation incorporating the known information: Then find the numbers of nucleons and charges necessary to balance the equation. In this instance, there are 238 nucleons on the left and 246 + 4 = 250 nucleons on the right, so the bombarding particle must have 250 – 238 = 12 nucleons. Furthermore, there are 92 nuclear charges on the left and 98 on the right, so the bombarding particle must have 98 – 92 = 6 protons. Solution The missing particle is .

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