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Nuclear Chemistry: Properties of Alpha, Beta, and Gamma RadiationGoals
BackgroundMost of the reactions studied in Chemistry 105 are chemical rather than nuclear in nature. This means that they involve motion of electrons surrounding stable nuclei. Because the nuclei do not change, and because the identity of an element is determined by the atomic number, Z, we can infer that in a typical chemical reaction the identities of the elements do not change. Any process in which the nucleus itself undergoes change and the identity of the element is altered is called a nuclear reaction. Nuclear reactions have important applications in chemistry and can be sources of enormous amounts of energy. The energy of the sun is generated by a nuclear reaction, the fusion of hydrogen nuclei into helium nuclei. Although nuclear reactions can be used in destructive ways, they have positive applications in the generation of electric power, in medical diagnosis, and in a variety of industrial applications. Despite the beneficial applications, the use of nuclear reactions continues to be controversial because all nuclear reactions produce by-products, including radiation and nuclear waste (unstable nuclei). In this lab, some of the fundamental properties of nuclear radiation will be studied to help you acquire a better understanding of the safety issues surrounding nuclear reactivity. All elements with atomic numbers greater than 83 are unstable. In addition, other nuclei can have an unstable mass:charge ratio. All unstable nuclei are said to be radioactive, meaning that they spontaneously disintegrate, or decay, into other nuclei. In this process, they typically emit electrons (beta particles, β), positrons (positive “electrons”, β+), or helium nuclei (alpha particles, α). Nuclear decay is sometimes accompanied by the emission of a photon of energy (electromagnetic radiation known as a gamma rays, γ). γ-ray emission does not affect the nuclear composition (number of protons and neutrons), but, rather, affects the energy of the nucleus. Alpha and beta particles and gamma rays are all ionizing radiation. As they pass through matter, they expend their energy by interacting with electrons on the molecules they encounter. In the process, electrons are ejected and reactive free radicals are formed. These free radicals can initiate chain reactions that disrupt previously stable systems. The properties of the three types of nuclear radiation that will be investigated are described below:
The product nucleus has an atomic number that is two less, and a mass number that is four less, than that of the original nucleus. Alpha particles are ejected with high energy. They efficiently ionize atoms in their path. They do not travel far but produce intense ionization within a short path. They travel at 5% to 7% of the speed of light.
An example of β-emission is the radioactive decay of carbon-14:
The product nucleus has an atomic number that is one more than that of the original nucleus. The mass number remains the same. With their high speed, up to 90% of the speed of light, single negative charge, and extremely small size and mass, the high energy β particles pass through matter much more easily than do a particles. The β particles are not monoenergetic and a spectrum of energies is obtained, with a characteristic maximum energy that corresponds to the actual energy transition in the nucleus. Radiation (α and β particles and γ-rays) is detected using a radiation monitor. The most familiar type of radiation monitor is a Geiger-Müller counter. High-energy radiation, such as α, β, or γ-radiation, enters through the window of the monitor and ionizes the argon gas enclosed within. The electrons and ions are attracted to positive and negative electrodes, respectively. This generates a small current flow between the electrodes. The current is amplified and used to activate a counter, a flashing light, and/or a clicking sound. The output of the counter can be directed to a computer for automated recording. Note: The Geiger counter measures "counts." These counts include both radiation from our sample of interest and some unavoidable background signal from other sources. We only care about the signal that comes from our sample, which we will call "activity": activity = counts – background Activity is a measure of radiation intensity, so activity and intensity can be used interchangeably. Synopsis of the ExperimentThis 2-part experiment will explore various properties of α, β, or γ-radiation. In Part I you will determine how well different types of radiation are blocked by physical barriers. You will measure the % transmission through paper and aluminum for each type of radiation, and compare their relative penetrating abilities. In Part II, you will determine whether or not physical separation (distance from a radiation source) is an effective way of protecting yourself from radiation. You will determine the relationship between intensity and distance for a γ-ray source. You will place a Geiger-Müller counter at different distances from a γ-emitter and measure counts at each distance. It is postulated that the intensity (I) of many physical properties, such as light or radioactivity, decreases as the distance (d) of the source (of light or radioactivity) from the detector increases. There are many possible relationships between (I) and (d), but we will narrow it down to one of the following three mathematical relationships:
All three equations have the general form of an equation of a line (y = mx + b), with x = 1/d2, d, or 1/d. Your task will be to plot your experimental data in three ways: I vs. 1/d2, I vs. d, and I vs. 1/d. The correct relationship should give a linear plot. The information that you obtain from the plots will allow you to determine the mathematical relationship between distance and intensity. PreparationEvery week, two items are due: Prelab for the current week and Results for the previous week. The Prelab and Results are in the form of worksheets, which are linked to in the Prelab & Results section, which is after the Experiment section of the lab manual.In order to prepare for the new lab each week, you should read the Background information section of the lab manual, any reading assignment found in the Preparation section, and the Experiment section. You should print the experiment section if you want a hard copy in lab. After the Experiment section, you should find your Prelab worksheet, which you should print, fill out, and turn in. You may also want to print the Results worksheet, so that you can work on it in lab if you have time.Reading Assignment:
Significant figures Significant figures is the number of digits reported, excluding zeroes to the left of the first nonzero number. When you report a measurement with correct significant figures, there will be some uncertainty in the last digit but the other digits are certain. There are two rules when determining significant figures in a calculated answer:
Scientific notation should be used for reporting answers whose significant figures are unclear (e.g. numbers rounded to the tens or hundreds place). When uncertainty is known, do not use the above rules for determining significant figures. Instead use the following rules:
Questions:Fill out the prelab worksheet that can be found at the end of the Experiment section. Print:Print and bring to lab: Look over, and print if you think it will be helpful:
Please print double-sided. ExperimentTo print instructions, select the portion that you wish to print, choose File/Print, and choose "selection" to prevent printing the entire web page.Safety
InstructionsStudents will work in groups of 2 unless otherwise specified by your instructor. There will be 2 stations set up, with different tasks to accomplish at each. All students must go through both stations. If there is no station available, start working on Workshop 2. For each station, you will be using sealed sources. These sources must be used with the label facing away from the detector (Why?). At each station, write down in your notebook which isotope your source contains (found on the label). Station I. Penetrating ability of α, β, and γ-radiationThe penetrating ability of α, β, and γ-radiation will be examined by quantitatively determining how much radiation is blocked by paper and aluminum for each type of source. You will measure 2 samples. For each sample, you will record one background reading (no sample), and three readings with different materials between the sample and the detector (air, paper, and aluminum). At Station I, a radiation counter fixed on top of a sample box will be used to measure radioactivity (see Figure 1) of an alpha, beta, or gamma radiation source.
The Geiger counter output will be read on a handset (see Figure 2). The counter has two displays. The upper display changes constantly, displaying the total number of radioactive events (“counts”) measured since the device was last turned on. At the end of a minute, the total number of counts measured during the that minute is displayed in the lower window. The upper display will continue to increase as more counts are measured, and the lower display will remain the same until another minute has passed. After you make a change to your setup (e.g. add paper between your source and detector), wait for the lower number to change. Disregard this number because it includes measurements made before your final setup. Wait one more minute and record the new number that appears in the lower display. Do not try to get around this problem by turning the counter off between measurements, because the first one-minute reading after turning the counter on is typically erroneous.
Record all of your data in your lab notebook as well as in the class spreadsheet, which will be posted on the lab conference. Results calculations will be performed on compiled class data. Each sample will have its own counter and sample box. To ensure that the class data is reliable, please do not move samples to different counters/boxes.
Station II. Intensity vs. distance relationshipThe activity of a γ-emitting sample will be measured at different distances from the radiation detector. The data will be interpreted to determine the relationship between γ-radiation intensity and distance. The sample and detector will be mounted on an alignment rail so that their separation distance can be readily adjusted. Refer to figures 3 and 4.
Workshop 2: Significant Figures, Statistical Uncertainty, and Plotting in ExcelLinks to reference materials: The workshop has three parts:
Prelab & ResultsClick here for Prelab worksheet: pdf or Word format Click here for Results worksheet: pdf or Word format A question to think about for your quiz:
Before Lab 3: Complete Safety Training
References1 Zumdahl, S.S.; Chemical Principles; Houghton Mifflin: Boston, New York, 5th ed., 2005. Use this reference for any future reading assignments that refer to Zumdahl Chase, G.D., Rituper, S., Sulcoski, J. W., Experiments in Nuclear Science, 2nd Ed., 1971. |
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Created By: Adilia James '07 and Sarah Coutlee '07 |