Handbook of Biochemistry
eBook - ePub

Handbook of Biochemistry

Section A Proteins, Volume III

  1. 633 pages
  2. English
  3. ePUB (mobile friendly)
  4. Available on iOS & Android
eBook - ePub

Handbook of Biochemistry

Section A Proteins, Volume III

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About This Book

This edition focuses solely on proteins, amino acids venom toxins and peptides, haemoglobin. It also gives us very detailed information regarding cell types, anti-bodies, infrared testing on protein cells and membrane studies.

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Publisher
CRC Press
Year
2018
ISBN
9781351089319
Proteins
OPTICAL ROTATORY DISPERSION AND CIRCULAR DICHROISM OF PROTEINS*
Jen Tsi Yang, G. Chi Chen, and Bruno Jirgensons
Biot in 1836 introduced the term specific rotation, [α], for the optical activity of a compound1, 2, 3
[ α ]λ = α/c
(1)
where
α
=
the observed rotation of the plane of polarized light in angular degrees at wavelength λ
=
the optical path in decimeters;
c
=
the concentration of the compound in grams per milliliter.
The dimension is deg cm2 decagram–1. The traditional use of specific rotation at sodium D line, [ α ]Dt, is now obsolete with the availability of modern spectropolarimeters. Here D refers to 589 nm and t the temperature in centigrade.
For biopolymers, the data are usually expressed in terms of mean residue rotation, [m]
[ m ] = (M0/100)[ α ]
(2)
where M0 is the mean residue (molecular) weight. (Some workers prefer the symbols [ϕ] or [R] for [m] and MRW for M0.) M0 of a protein can be determined from its amino acid composition (for most proteins, M0 ≅ 115). Moffitt4 introduced the term reduced mean residue rotation, [m′], by including a Lorentz field correction
[ m]=[ m ][ 3/(n2+2) ]
(3)
which reduces [m] to that under vacuum, noting that the refractive index is unity in vacuum. The dimension of both [m] and [m′] is deg cm2 dmol−1.
Optical rotatory dispersion (ORD) in the visible region of most proteins obeys the Drude equation
[ α ]λ = k/(λ2 λc2)
(4)
where λc and k are the dispersion and rotatory coefficients. A plot of λ2 [α]λ vs. [α]λ yields a straight line with λc2 as the slope and k as the intercept (at [α]λ = 0).5 The Moffitt equation for α-helical polypeptides4
[ m]=a0λ02/(λ2λ02)+b0λ04/(λ2λ02)2
(5)
has now replaced the Drude equation for the ORD of proteins (except collagen). By rearranging Equation 5 into
[ m](λ2/λ021)=a0+b0/(λ2/λ021)
(6)
the b0 and a0of a protein can be determined from a plot of [m’](λ202 – 1) vs. 1/(λ202 – 1) with λ0 usually preset at 212 nm. A b0 of-630 deg cm2 dmol−1, based on the data of synthetic polypeptides, is regarded to represent a perfect helix. The Moffitt equation, now considered to be empirical, still provides a reasonable estimate of the helical content in a protein molecule. Both Equations 4 and 5 are only applicable over a certain wavelength range. Often a λ0 larger than 212 nm must be used when the data below 300 to 350 nm are included for the fitting of the Moffitt equation. For the convenience of comparison, we will list only the a0 and b0 values based on λ0 = 212 nm (with a few exceptions).
The visible ORD can also be fitted with many two-term Drude equations
[ m]=a1λ12/(λ2λ22)+a2λ22/(λ2λ22)
(7)
One such equation has been proposed by Shechter and Blout6 with λ1 = 193 and λ2 = 225 nm. All these equations can be reduced to the Moffitt equ...

Table of contents

  1. Cover
  2. Half Title
  3. Title Page
  4. Copyright Page
  5. Dedication
  6. Table of Contents
  7. PROTEINS
  8. INDEX