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Biomedical

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Title: Biomedical


1
Biomedical Biophysics Research at
TcSUHElectromagnetic Properties of Biological
Systems
  • John H. Miller, Jr.
  • Department of Physics and
  • Texas Center for Superconductivity
  • University of Houston
  • Summer 2005 Houston Quarknet Workshop
  • June 24, 2005

2
Fundamental Principles of biological systems
  • Emergence
  • Higher organizing principles emerge independently
    of the details of the microscopic Hamiltonian.
    (Anderson, Laughlin, Pines).
  • Information Bioinformatics
  • Biological systems carry, preserve, and replicate
    information. Information is encoded via genetic
    code, sugar code, histone code, splicing code,
    gene regulation code ...
  • Convergent increase in complexity
  • The information content in an organism is vastly
    greater than that of its genome.
  • Natural Selection Evolution
  • Similar principles may extend to non-biological
    systems (eg. language, music, culture). In
    biology, evolution is partly driven by mutations.

3
Fundamental Principles (continued)
  • Metabolism Bioenergetics
  • Living systems consume free energy U TS. The
    total energy is conserved (Uin Uout) so Sin ltlt
    Sout. Organisms consume negative entropy - S
    k log (1/Nstates). (Schrödinger What is
    Life.)
  • Quantum Protectorate
  • Quantum mechanics plays a crucial role in
    preserving information. Discrete gaps between
    energy levels enable stability of molecules (DNA,
    proteins, etc.). Lifetime of a molecule can be
    long t texpD/kT, so at T 300 K, if D
    1.8 eV, then t 30,000 years.
  • Biological systems are complex, dynamically
    evolving materials.
  • Condensed matter physics phenomena include
    diamagnetism, charge density waves, dielectric
    response, ferroelectricity, piezoelectricity,
    quantum tunneling, excitons, and proposed
    biological superconductivity.

4
Electromagnetic Interactions are vital to living
systems.
  • Electromagnetism is dominant in chemical and
    biological processes.
  • Biological macromolecules (in water) are highly
    charged /or have
  • strong electric dipole moments.
  • Both repulsion and attraction (eg. in presence
    of Ca2) can occur
  • between like charged polyelectrolytes.
  • Electromagnetic interactions can be extended to
    long distances by
  • charge density waves, microtubules, etc.
  • Live cells exhibit electromotility, especially
    outer hair cells.

5
Effects of an external electric field
  • At low frequencies, most of the potential drop
    is across the plasma
  • membrane.
  • Induced potential Um(w,q) 1.5 E0R cosq 1
    iwtm.
  • 5 V/cm field ? Um 15mV for a 20mm radius cell.

6
Oscillatory field affects membrane proteins.
  • AC fields can actually drive cation transport in
    membrane pumps,
  • even in the absence of ATP (Tsong, Astumian,
    et al).
  • Oscillatory fields also induce conformational
    changes.
  • Resulting motion of electric dipoles and charges
    generates harmonics.

7
P-type ATPases
8
Nonlinear response Measurement of induced
harmonics
  • A sinusoidal electric field is applied to the
    cell suspension.
  • At low frequencies (lt 1 kHz) we use a SQUID to
    probe the currents.
  • A spectrum of harmonics, induced by membrane
    pumps, is recorded.
  • (Nawarathna et al, APL 2004)

9
Probing membrane pumps in yeast cells
3 V/cm
23 Hz
10
Harmonic response of yeast after adding glucose
45 Hz
3 V/cm
11
Asymmetric Junction Model
  • AC voltage drives conformational changes cation
    transport.
  • Threshold voltages, V1 V2, and time scales, t1
    t2.

12
Can probe internal organelles at kHz freqs.
13
Probing the mitochondrial electron transport chain
Nonlinear harmonic response
Peaks are suppressed by adding potassium cyanide.
14
Electron Transfer via Quantum Tunneling
Pathway for ET from cytochrome c to active site
of CcO
For a recent review see A. A. Stuchebrukhov,
Long-distance electron tunneling in proteins,
Theoretical Chem. Accounts, 110, 291
(2003). Discovery of activationless ET DeVault
Chance (1966) Theory of ET reactions Rudolph
Marcus (Nobel Prize in Chem. 1992)
Pilet et al. (2004) PNAS 101, 16198
Protein environment of the heme rings a and a3.
The dominant ET pathway from heme a to a3 is
shown as a dotted line. (Tan et al., BPJ 86, 1813
(2004)) Iron atom in heme a e- queing point
feeds 4 e-s into an O2 molecule held at the Cu
Fe active site at heme a3. 4e- 4H O2 ? 2H2O
15
Probing the electron transport chain in
chloroplasts
16
Photosynthetic electron transport chain
17
Charge Density Waves
(A) Uncondensed and (B) condensed F-actin,
mediated by charge-density wave of divalent
cations. T. E. Angelini, et al. PNAS 100, 8634
(2003). Charge density waves also proposed to
form in membranes.
18
Microtubules
Anisotropic diamagnetism reported for
microtubules. MTs also proposed to be
ferroelectric.
a-b tubulin dimer
MT cytoskeleton
Very large dipole moment! 1500 debye 5 x
10-27 C m.
A microtubule may act as a ferroelectric with a
melting temp. of 57ºC. Brown Tuszynski,
Phys. Rev. E 56, 5834 (1997).
19
Microtubules Electrostatic Interactions
MTs radiating from centrosome
Analogy Electrostatic repulsion of hair.
MT growth
1. During mitosis
Nanoscale electrostatics may play a key role in
prometaphase, metaphase, and anaphase-A. Intracel
lular pH peaks during mitosis. L. J. Gagliardi,
J. Electrostatics 54, 219 (2002).
2. After depolymerization (Moscow State
University)
Artificial mitotic spindle, R. Heald, et al.
(1996) Nature 382, 420-425.
20
Live cells proteins show dielectric
responses that decrease with frequency.
21
Tubulin dimer suspensions show strong dielectric
response.
Free tubulin dimers become frozen out as they
polymerize (self-assemble) to form microtubules
when T gt 0º C. ? Reduced concentration of free
dimers.
22
Tubulin dimer suspensions conductivity vs.
frequency.
23
PrestinA Membrane Protein Involved in OHC
Electromotility
Has 12 transmembrane domains may form a
tetramer high density (1/(20nm2)) in membrane.
  • Mediates OHC length changes
  • to tune hearing frequencies
  • has homology with sulfate transporters
  • operates at microsecond rates up to 100 kHz
  • voltage-to-force converter
  • Electromotility
  • Cochlear amplifier
  • Incomplete anion transporter

Zheng et al, Nature 405, 149 (2000). P. Dallos
B. Fakler, 2002
24
Linear dielectric response Prestin-transfected
yeast vs. control.
We see slight differences between S. cerevisiae
expressing prestin vs. control samples. Miller
et al., J. Biological Physics 2005.
D ep(f)/ep(ff0) - ec(f)/ec(f0).
Frequency range appears consistent w/ OHC
piezoelectric resonances. Rabbitt et al. 2004.
25
Other CMP Phenomena Diamagnetism
High Field Magnet Lab University of Nijmegen
Partly due to disipationless screening currents
in aromatic rings.
Anisotropic diamagnetism in microtubules, actin,
fibrin.
Lowest energy p orbital of an aromatic ring,
constructed from a superposition of pz-orbitals.
The p-electron moves freely in a torus following
the conjugation path of the molecule.
26
Biomedical Applications Biomagnetism
  • Magnetic fields produced by action potentials
  • Magnetoencephalography (MEG), MCG, MGG, MMG,
    MRG, etc.

27
Impedance Magnetocardiography (I-MCG)
  • ECG measures the electrical potentials generated
    by bioelectric currents in the heart.
  • MCG measures the weak magnetic fields due to
    bioelectric currents resulting from the
    propagating action potentials in the heart (eg.
    A. Brazdeikis)
  • I-MCG measures changes in impedance during the
    cardiac cycle due, in part, to changes in blood
    volume. Can probe cardiac ejection fraction and
    other properties.

28
I-MCG Setup
Noise measurements inside and outside the shield
29
I-MCG recording using High-Tc SQUID
30
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31
Magnetic Resonance Imaging (MRI)
32
MRI Twin-Horseshoe HTS 2-T Receiver Probe
(84.4 MHz, J. Wosik)
Patterned on a double sided 2 YBCO film on
LaAlO3
The probe inside a plastic liquid nitrogen
cryostat
33
MRI 2-Tesla MR Image of Rat
spinal-cord
4 dB gain
brain
34
Conclusions
  • Physics concepts can contribute to understanding
    of biological processes and lead to biomedical
    applications.
  • Experimental tools of condensed matter physics
    and materials science can play an important role
    in characterizing biological systems.

35
Acknowledgements
  • University of Houston
  • Jarek Wosik (MRI), Audrius Brazdeikis (MCG),
    D. Nawarathna, Hugo Sanabria, Vijay Vajrala,
    James Claycomb, Gustavo Cardenas, David
    Warmflash, Jarek Wosik, William Widger, Jeffrey
    Gardner
  • Baylor College of Medicine
  • William Brownell, Fred Pereira
  • Funding
  • TcSUH, Welch Foundation,
  • NASA-ISSO
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