By Hiroyuki Ohshima
Chapter 1 strength and cost of a difficult Particle (pages 1–46):
Chapter 2 strength Distribution round a Nonuniformly Charged floor and Discrete cost results (pages 47–62):
Chapter three transformed Poisson?Boltzmann Equation (pages 63–82):
Chapter four capability and cost of a smooth Particle (pages 83–110):
Chapter five unfastened strength of a Charged floor (pages 111–131):
Chapter 6 capability Distribution round a Charged Particle in a Salt?Free Medium (pages 132–162):
Chapter 7 Electrostatic interplay of aspect fees in an Inhomogeneous Medium (pages 163–185):
Chapter eight strength and strength power of the Double?Layer interplay among Charged Colloidal debris (pages 186–202):
Chapter nine Double?Layer interplay among Parallel comparable Plates (pages 203–240):
Chapter 10 Electrostatic interplay among Parallel varied Plates (pages 241–264):
Chapter eleven Linear Superposition Approximation for the Double?Layer interplay of debris at huge Separations (pages 265–282):
Chapter 12 Derjaguin's Approximation at Small Separations (pages 283–297):
Chapter thirteen Donnan Potential?Regulated interplay among Porous debris (pages 298–322):
Chapter 14 sequence growth Representations for the Double?Layer interplay among debris (pages 323–356):
Chapter 15 Electrostatic interplay among tender debris (pages 357–374):
Chapter sixteen Electrostatic interplay among Nonuniformly Charged Membranes (pages 375–380):
Chapter 17 Electrostatic Repulsion among Parallel delicate Plates after their touch (pages 381–387):
Chapter 18 Electrostatic interplay among Ion?Penetrable Membranes in a Salt?Free Medium (pages 388–398):
Chapter 19 van der Waals interplay among debris (pages 399–419):
Chapter 20 DLVO concept of Colloid balance (pages 420–430):
Chapter 21 Electrophoretic Mobility of soppy debris (pages 431–467):
Chapter 22 Electrophoretic Mobility of focused delicate debris (pages 468–479):
Chapter 23 electric Conductivity of a Suspension of sentimental debris (pages 480–484):
Chapter 24 Sedimentation strength and speed in a Suspension of sentimental debris (pages 485–496):
Chapter 25 Dynamic Electrophoretic Mobility of a tender Particle (pages 497–507):
Chapter 26 Colloid Vibration capability in a Suspension of sentimental debris (pages 508–514):
Chapter 27 potent Viscosity of a Suspension of soppy debris (pages 515–532):
Chapter 28 Membrane strength and Donnan capability (pages 533–542):
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Additional info for Biophysical Chemistry of Biointerfaces
From Ref. 5.
18 shows equipotential lines (contours) around a prolate spheroid on the z–x plane at y ¼ 0, calculated from Eq. 5 and kb ¼ 1. 18 Equipotential lines (contours) around a prolate spheroid on the z–x plane at y ¼ 0. Calculated from Eq. 5 and kb ¼ 1 (arbitrary size). REFERENCES 45 We next consider the case of an oblate spheroid with constant surface potential co (Fig. 17b). The surface of the oblate is given by x2 þ y 2 z2 þ 2¼1 a2 b ð1:213Þ where the z-axis is again the axis of symmetry, a and b are the major and minor semiaxes, respectively.
88). As another example, one can derive expressions for the s–yo relationship for the case of 3-1 electrolytes of concentration n. In this case, the Debye–Hu¨ckel parameter k and f(y) are given by Eqs. 62), respectively. By substituting Eq. 62) into Eqs. 109) and carrying out numerical integration, we can derive the first-order and second-order s–yo relationships, respectively. The relative error of Eq. 103) is less than 1% for ka ! 5 and that of Eq. 109) is less than 1% for ka ! 1. 5 Potential Distribution Around a Sphere with Arbitrary Potential By using an approximation method similar to the above method and the method of White , one can derive an accurate analytic expression for the potential distribution around a spherical particle.
Biophysical Chemistry of Biointerfaces by Hiroyuki Ohshima