/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 10 Technetium-99 (æ?r) has an exci... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

Technetium-99 (æ?r) has an excited state that decays by emission of a gamma ray. The half-life of the excited state is 360 min. What is the activity, in curies, of \(1.00 \mathrm{mg}\) of this excited isotope? Because we have the half-life \(\left(t_{1 / 2}\right)\) we can determine the decay constant since \(\lambda t_{1 / 2}=0.693 .\) The activity of a sample is \(\lambda N .\) In this case, $$ \lambda=\frac{0.693}{t_{1 / 2}}=\frac{0.693}{21600 \mathrm{~s}}=3.21 \times 10^{-5} \mathrm{~s}^{-1} $$ We also know that \(99.0 \mathrm{~kg}\) of Tc contains \(6.02 \times 10^{26}\) atoms. A mass \(m\) will therefore contain \([m /(99.0 \mathrm{~kg})]\left(6.02 \times 10^{26}\right)\) atoms. In our case, \(m=1.00 \times 10^{-6} \mathrm{~kg}\), and so $$ \begin{aligned} \text { Activity } &=\lambda N=\left(3.21 \times 10^{-5} \mathrm{~s}^{-1}\right)\left(\frac{1.00 \times 10^{-6} \mathrm{~kg}}{99.0 \mathrm{~kg}}\right)\left(6.02 \times 10^{26}\right) \\ &=1.95 \times 10^{14} \mathrm{~s}^{-1}=1.95 \times 10^{14} \mathrm{~Bq} \end{aligned} $$

Short Answer

Expert verified
The activity is 5.27 curies.

Step by step solution

01

Determine the decay constant

First, calculate the decay constant \( \lambda \) using the half-life formula: \( \lambda t_{1/2} = 0.693 \). Given \( t_{1/2} = 360 \text{ mins} = 21600 \text{ s} \), thus \( \lambda = \frac{0.693}{21600 \text{ s}} = 3.21 \times 10^{-5} \text{ s}^{-1} \).
02

Calculate the number of atoms in the sample

We know \(99.0 \text{ kg}\) of Tc contains \(6.02 \times 10^{26}\) atoms. For a mass \(m = 1.00 \times 10^{-6} \text{ kg (1 mg)} \), the number of atoms \(N\) is \( \left(\frac{1.00 \times 10^{-6} \text{ kg}}{99.0 \text{ kg}}\right) \times 6.02 \times 10^{26} = 6.08 \times 10^{18}\).
03

Calculate the activity in becquerels

Use the formula for activity \(A = \lambda N\): \(A = (3.21 \times 10^{-5} \text{ s}^{-1}) \times 6.08 \times 10^{18} = 1.95 \times 10^{14} \text{ Bq}\).
04

Convert becquerels to curies

Finally, convert the activity from becquerels to curies. Since \(1\text{ Ci} = 3.7 \times 10^{10}\text{ Bq}\), the activity in curies is \(\frac{1.95 \times 10^{14} \text{ Bq}}{3.7 \times 10^{10} \text{ Bq/Ci}} = 5.27 \text{ Ci}\).

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with 91Ó°ÊÓ!

Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Decay Constant Calculation
The decay constant, denoted as \( \lambda \), is a fundamental concept in radioactive decay. It represents the probability per unit time that a given nucleus will decay. Understanding \( \lambda \) is crucial, as it connects the half-life of a radioactive isotope with its decay kinetics.
To calculate the decay constant \( \lambda \) from the half-life \( t_{1/2} \), use the formula:
  • \( \lambda = \frac{0.693}{t_{1/2}} \)
The factor 0.693 is derived from the natural logarithm of 2 (ln(2)), which relates to the exponential nature of decay.
In practical terms, if you know the half-life of an isotope, just divide 0.693 by the half-life (converted to the desired unit) to find \( \lambda \). For example, if Technetium-99's half-life is 360 minutes, convert that time to seconds for uniformity. Then, calculate \( \lambda \) by plugging into the formula to get \( \lambda = 3.21 \times 10^{-5} \text{ s}^{-1} \). This conversion ensures \( \lambda \) is in units \( \text{s}^{-1} \), which is standard for decay constants.
Half-Life
The half-life of a radioactive substance is the time it takes for half of the radioactive nuclei in a sample to decay. It is an essential aspect in nuclear physics, as it provides insight into the rate at which a isotope disintegrates.
Half-life is often used in a variety of applications such as radiometric dating, medicine, and nuclear power. It is unique to each isotope and remains constant over the isotope's lifetime. Understanding half-life helps quantify and predict the long-term behavior of radioactive substances.
Since half-life (\( t_{1/2} \)) is related inversely to the decay constant, they are used interchangeably to describe the rate of decay. For Technetium-99, a half-life of 360 minutes (or 6 hours) tells us that after 6 hours, only half of the initial amount of the isotope will remain radioactive.
Activity Calculation
The concept of "activity" in radioactive materials pertains to how many atoms in a sample decay per unit of time. It's often expressed in terms of becquerels (Bq) or curies (Ci), reflecting the intensity of the radioactive substance.
Activity (\( A \)) is calculated using the formula:
  • \( A = \lambda N \)
where \( N \) is the number of radioactive atoms present and \( \lambda \) is the decay constant.
In the case of our example with Technetium-99, once you have determined \( \lambda = 3.21 \times 10^{-5} \text{ s}^{-1} \) and know \( N \) (or number of atoms), you can calculate activity. By plugging the values, you determine the sample's activity in becquerels, which can be further converted to curies using the conversion factor \( 1 \text{ Ci} = 3.7 \times 10^{10} \text{ Bq} \). This conversion is particularly useful in contexts where traditional units like curies are preferred over becquerels, such as in the medical field.

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

By how much does the mass of a heavy nucleus change when it emits a 4.8-MeV gamma ray?

Suppose we bombard nitrogen with alpha particles. What might result if an alpha is absorbed and a proton subsequently is emitted? [Hint: Write out an equation accounting for all the particles.]

The half-life of radium is \(1.62 \times 10^{3}\) years. How many radium atoms decay in \(1.00 \mathrm{~s}\) in a \(1.00 \mathrm{~g}\) sample of radium? The atomic weight of radium is \(226 \mathrm{~kg} / \mathrm{kmol}\). A 1.00-g sample is \(0.00100 \mathrm{~kg}\), which for radium of atomic number 226 is \((0.00100 / 226)\) kmol. Since each kilomole contains \(6.02 \times 10^{26}\) atoms, $$ N=\left(\frac{0.00100}{226} \mathrm{kmol}\right)\left(6.02 \times 10^{26} \frac{\text { atoms }}{\mathrm{kmol}}\right)=2.66 \times 10^{21} \text { atoms } $$ The decar constanti Then $$ \begin{array}{l} \lambda=\frac{0.693}{t_{1 / 2}}=\frac{0.693}{(1620 y)\left(3.156 \times 10^{7} \mathrm{~s} / \mathrm{y}\right)}=1.36 \times 10^{-11} \mathrm{~s}^{-1} \\ \frac{\Delta N}{\Delta t}=\lambda N=\left(1.36 \times 10^{-11} \mathrm{~s}^{-1}\right)\left(2.66 \times 10^{21}\right)=3.61 \times 10^{10} \mathrm{~s}^{-1} \end{array} $$ is the number of disintegrations per second in \(1.00 \mathrm{~g}\) of radium. The above result leads to the definition of the curie (Ci) as a unit of activity: \(1 \mathrm{Ci}=3.7 \times 10^{10}\) disintegrations/s \(/ \mathrm{s}\) Because of its convenient size, we shall sometimes use the curie in subsequent problems, even though the official SI unit of activity is the becquerel.

An experiment is done to determine the half-life of a radioactive substance that emits one beta particle for each decay process. Measurements show that an average of \(8.4\) beta particles are emitted each second by \(2.5 \mathrm{mg}\) of the substance. The atomic mass of the substance is \(230 .\) Find the half- life of the substance.

How many protons, neutrons, and electrons are there in \((a){ }^{3} \mathrm{He}\), (b) \(^{12} \mathrm{C}\), and \((c)^{206} \mathrm{~Pb}\) ? (a) The atomic number of He is 2; therefore, the nucleus must contain 2 protons. Since the mass number of this isotope is 3 , the sum of the protons and neutrons in the nucleus must equal 3; therefore, there is 1 neutron. The number of electrons in the atom is the same as the atomic number, 2 . (b) The atomic number of carbon is 6 ; hence, the nucleus must contain 6 protons. The number of neutrons in the nucleus is equal to \(12-6=6\). The number of electrons is the same as the atomic number, 6 . (c) The atomic number of lead is 82 ; hence, there are 82 protons in the nucleus and 82 electrons in the atom. The number of neutrons is \(206-82=124\).

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.