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Related Concept Videos

Proton (¹H) NMR: Chemical Shift01:07

Proton (¹H) NMR: Chemical Shift

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Organic molecules primarily contain carbon and hydrogen atoms. While all the hydrogen isotopes are NMR-active, protium or hydrogen-1 is the most abundant. It has a significant energy separation between its nuclear spin states due to its large gyromagnetic ratio. As per Boltzmann's distribution, an increase in the energy separation implies a greater excess population of nuclei available for excitation, resulting in a strong NMR absorption signal.
Absorption signals of all the protium nuclei...
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¹H NMR: Complex Splitting01:13

¹H NMR: Complex Splitting

1.5K
A proton M that is coupled to a proton X results in doublet signals for M. However, NMR-active nuclei can be simultaneously coupled to more than one nonequivalent nucleus. When M is coupled to a second proton A, such as in styrene oxide, each peak in the doublet is split into another doublet.
Splitting diagrams or splitting tree diagrams are routinely used to depict such complex couplings. While drawing splitting diagrams, the splitting with the larger coupling constant is usually applied...
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¹H NMR Chemical Shift Equivalence: Homotopic and Heterotopic Protons01:03

¹H NMR Chemical Shift Equivalence: Homotopic and Heterotopic Protons

3.7K
Protons in identical electronic environments within a molecule are chemically equivalent and have the same chemical shift. The replacement test is a useful tool to identify chemical equivalence and predict NMR spectra. A substituent replaces each of the protons being examined and the resulting molecules are compared. If the same molecule is obtained, the protons are equivalent or homotopic. Replacement of any hydrogens in ethane by chlorine yields chloroethane because all six protons are...
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Molecular Models02:00

Molecular Models

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Physical models representing molecular architectures of chemical compounds play essential roles in understanding chemistry. The use of molecular models makes it easier to visualize the structures and shapes of atoms and molecules.
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The Bohr Model02:18

The Bohr Model

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Following the work of Ernest Rutherford and his colleagues in the early twentieth century, the picture of atoms consisting of tiny dense nuclei surrounded by lighter and even tinier electrons continually moving about the nucleus was well established. This picture was called the planetary model since it pictured the atom as a miniature “solar system” with the electrons orbiting the nucleus like planets orbiting the sun. The simplest atom is hydrogen, consisting of a single proton as the...
78.0K
Interpreting ¹H NMR Signal Splitting: The (n + 1) Rule01:10

Interpreting ¹H NMR Signal Splitting: The (n + 1) Rule

2.1K
In the AX proton spin system, proton A can sense the two spin states of a coupled proton X, resulting in a doublet NMR signal with two peaks of equal (1:1) intensity. When proton A is coupled to two equivalent protons (AX2 spin system), the spin states of each X can be aligned with or against the external field, creating three possible scenarios. This results in a 1:2:1  triplet signal, where the central peak corresponds to the chemical shift of A and is twice as large or intense as the...
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Proton Therapy Delivery and Its Clinical Application in Select Solid Tumor Malignancies
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Proton RBE models: commonalities and differences.

Stephen J McMahon1

  • 1Patrick G Johnston Centre for Cancer Research, Queen's University Belfast, Belfast, BT9 7AE, United Kingdom.

Physics in Medicine and Biology
|January 11, 2021
PubMed
Summary
This summary is machine-generated.

Proton therapy

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Area of Science:

  • Medical Physics
  • Radiation Oncology
  • Radiobiology

Background:

  • Relative biological effectiveness (RBE) of protons is crucial for optimizing proton therapy.
  • Current treatment planning often uses a fixed RBE of 1.1, despite preclinical data showing variability.
  • Existing phenomenological models for proton RBE show poor agreement, hindering clinical application.

Purpose of the Study:

  • To investigate conceptual agreement and disagreement among different proton RBE models.
  • To identify key parameters driving discrepancies between these models.
  • To guide future research for more accurate RBE modeling in proton therapy.

Main Methods:

  • Comparative analysis of phenomenological proton RBE models.
  • Evaluation of model predictions across varying biological and physical parameters.
  • Focus on linear energy transfer (LET) dependence and linear-quadratic model parameters (α and β).

Main Results:

  • Primary model disagreements stem from the handling of biological parameters (α and β) from the linear-quadratic model.
  • All models demonstrate strong correlation when analyzed for dependence on linear energy transfer (LET).
  • Conceptual agreement is observed regarding LET-dependence, but differences in biological parameter handling persist.

Conclusions:

  • Systematic exploration of biological variation in RBE is needed.
  • Well-controlled studies across diverse cell types are essential.
  • Distinguishing between models requires a focus on biological parameter differences and validation against experimental data.