Lecture 3 Flashcards

1
Q
  • Name 3 systems that produce isotropic EPR spectra
A
    1. Unpaired electron in an s orbital. Spherically symmetric therefore probability of finding electron/radical same regardless of direction of magnetic field
    1. Sample tumbling rapidly in solution. Direction doesn’t matter as averages over all possible directions
    1. Unpaired electrons is in a cubic symmetry environment
  • All result in orientation independent/symmetric EPR spectra that are simple to analyse.
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2
Q
  • Sketch the line shape for S= 1/2, I = 0 powder EPR spectrum that would be the result of an isotropically symmetric system.
A
  • Any magnetic field, B direction results in derivative of resonance in exact same position as no anisotropy present
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3
Q
  • Describe the origin of anisotropy in terms of the g-tensor associated with the Hamiltonian of the hyperfine energy
A
  • Deviation from g tensor associated with free electron spin where system xyz chosen such that diagonal gxx/gyy/gzz elements relevant in Hamiltonian describing hyperfine energy
  • In an isotropic system, orientation dependence of g tensor values are averaged by fast molecular motion and an isotropic g-value is observed
  • giso = 1/3(gxx + gyy + gzz)
  • As tumbling not present in anisotropic system, how the magnetic field aligns with the axis of the non-symmetric (e.g. p-orbital) will change the contribution to the overall g value
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4
Q
  • Describe the origin of gII/gT terms of a radical in a p orbital in a magnetic field
A
  • Position of resonance when orbital aligned parallel to magnetic field (z-axis) –> gz/gII
  • Position of resonance when orbital aligned perpendicular to magnetic field (x/y-axis –> gx,y/gT
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5
Q
  • Sketch the line shape for S= 1/2, I = 0 powder EPR spectrum that would be the result of an axially symmetric system.
A
  • Field modulation used to encode signal and lock in detect out gradient of line (higher sensitivity)
  • This is a solid state powder spectrum os a system where no tumbling is occurring and is anisotropic and axially symmetric, and likely a radical in a p-orbital
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6
Q
  • Explain the intensities of the S= 1/2 , I=0 powder spectrum of an axially symmetric system
A
  • Intensity is due to probability of spins aligning with magnetic field, B depending on orientation
  • When aligned parallel with B (along z-axis), there is a low probability of spins being aligned where a radical is frozen in solution at this orientation
  • Results in the gII factor
  • When aligned perpendicular to magentc field, B a higher intensity arises as more likely for a spin to be aligned anywhere in the xy plane relative to B
  • Results in the gT factor
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7
Q
  • How does the magnitude of a g factor in a powder spectrum relate to the magnetic field, B?
A
  • g = hv/µBB
  • Therefore, g varies inversely with B
  • A low g factor occurs at a high field
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8
Q
  • What are the three types of powder EPR spectra and their conditions
A
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9
Q
  • Sketch an absorption and first derivative powder spectrum for an axial and orthorhombic system with labelled corresponding g values
A
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