Friday, January 13, 2017

CHEM 418 Nuclear Chemistry, Winter 2017: Lecture 4 Alpha Decay

This lecture discusses alpha decay in radionuclides.  Theories on alpha decay are presented. Systematics and energetics involved in alpha decay are presented.  The correlation between Q value and decay energy is described.  The Geiger Nuttall relationship is provided, described, and utilized in a model for alpha decay. Tunneling is also exploited to described alpha decay, coupling energy and half-life.  Gamow calculations are shown to reflect the Geiger Nuttall relationship. Hindered alpha decay is discussed. Hindered alpha decay is employed to described nuclear properties. Hinderance factors are described, along with how they are calculated and where they can be found. Proton and other charged particle emission are presented. The lecture time is 50 minutes.  The lecture is assigned on Friday 13 January 2017 and due Wednesday 18 January 2017. 

13 comments:

  1. thanks for the submitted PDF quiz 4.

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  2. For quiz 4, I found there are two 244Cm on question 1.

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  3. Thanks. I will review and correct question 1.

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  4. Note on question 1. The isotope 244Cm appears twice. This does not impact the correct answer in the PDF quiz.

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  5. Lecture viewed and pdf quiz 4 submitted via e-mail.

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    1. thanks for your reply. Please see my e-mail response.

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  6. Lecture 4 has been reviewed and the PDF quiz 4 has been submitted.

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  7. Lecture and quiz 4 viewed and submitted

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  8. Lecture was viewed and Quiz 4 submitted. I apologize for the late submission.

    Could you expand on obtaining the "lower" kinetic energy of emitted alpha particle and using it to determine velocity of alpha particle in the nucleus?

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    1. The alpha particle velocity is 1/2mv^2. The kinetic energy of the emitted alpha particle can be used to calculate the particle velocity. Depending upon the specific isotope, the alpha decay may have different energies. This velocity, combined with information on the nuclear radius, can be used to calculate how often the particle traverses the nucleus prior to emission.

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