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32.3 Therapeutic Uses of Ionizing Radiation

Killing tumor cells with external gamma and beam doses or implanted sources, and the dose levels in grays that cancer treatment actually delivers.

College Physics 2e, 32.3 Therapeutic Uses of Ionizing Radiation

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5 exercises

32.3 Exercise 2

A beam of 168-MeV nitrogen nuclei is used for cancer therapy. If this beam is directed onto a 0.200-kg tumor and gives it a 2.00-Sv dose, how many nitrogen nuclei were stopped? (Use an RBE of 20 for heavy ions.)

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32.3 Exercise 4

Calculate the dose in Sv to the chest of a patient given an x-ray under the following conditions. The x-ray beam intensity is 1.50 W/m2\text{1}.\text{50 W} /\text{m}^{2}, the area of the chest exposed is 0.0750m2\text{0}.\text{0750} \text{m}^{2}, 35.0% of the x-rays are absorbed in 20.0 kg of tissue, and the exposure time is 0.250 s.

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32.3 Exercise 6

What is the mass of 60Co^{60} \text{Co} in a cancer therapy transillumination unit containing 5.00 kCi of 60Co^{60} \text{Co}?

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32.3 Exercise 8

Naturally occurring 40K^{\text{40}} \text{K} is listed as responsible for 16 mrem/y of background radiation. Calculate the mass of 40K^{\text{40}} \text{K} that must be inside the 55-kg body of a woman to produce this dose. Each 40K^{\text{40}} \text{K} decay emits a 1.32-MeV β\beta, and 50% of the energy is absorbed inside the body.

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32.3 Exercise 10

The annual radiation dose from 14C^{14} \text{C} in our bodies is 0.01 mSv/y. Each 14C^{14} \text{C} decay emits a β–\beta^{–} averaging 0.0750 MeV. Taking the fraction of 14C^{14} \text{C} to be 1.3×10–12N1.3 \times 10^{–12} \text{N} of normal 12C^{12} \text{C}, and assuming the body is 13% carbon, estimate the fraction of the decay energy absorbed. (The rest escapes, exposing those close to you.)

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Adapted from College Physics © 2022 Rice University. Licensed under CC BY 4.0. Sources: College Physics 2e, College Physics for AP® Courses 2e. Imported at revision f98d7a7.