Related Experiment Video
Updated: Jul 19, 2025

08:23
Finite Element Modelling of a Cellular Electric Microenvironment
Published on: May 18, 2021
3.5K
The pH dependent surface charging and points of zero charge. X. Update
1Lublin University of Technology, Nadbystrzycka 38, PL-20618 Lublin, Poland.
Advances in Colloid and Interface Science
|August 13, 2023
Summary
This review compiles accurate surface charge data, focusing on points of zero charge (PZC) and isoelectric points (IEP) determined using reliable methods with inert electrolytes. It clarifies terminology and presents new and older data for materials science.
Area of Science:
- Surface Chemistry
- Materials Science
- Electrochemistry
Background:
- Surface properties like points of zero charge (PZC) and isoelectric points (IEP) are crucial but often ambiguously defined and measured.
- Existing literature shows inconsistent terminology and methodology for determining these surface characteristics.
Purpose of the Study:
- To critically review and compile accurate PZC and IEP data for various materials.
- To standardize the definition and measurement of PZC and IEP, focusing on inert electrolyte conditions.
- To present recent findings alongside previously overlooked data for comprehensive comparison.
Main Methods:
- Focusing on PZC determination via potentiometric titration curves at multiple ionic strengths.
- Including IEP data for diverse materials.
- Excluding results from less rigorous methods like mass titration or pH-drift.
Main Results:
- Compilation of PZC/IEP data obtained under specific conditions (inert electrolytes, controlled temperature).
- Inclusion of data for metal oxides and other materials.
- Cross-referencing with previous reviews for historical data comparison.
Conclusions:
- Clarifies the precise definitions and reliable measurement techniques for PZC and IEP.
- Provides a valuable, updated resource for researchers in surface science and materials.
- Highlights the importance of consistent methodology for accurate surface characterization.
Related Concept Videos
Potential Due to a Polarized Object
434
A neutral atom consists of a positively charged nucleus surrounded by a negatively charged electron cloud. When placed in an external electric field, the external electric force pulls the electrons and nucleus apart, opposite to the intrinsic attraction between the nucleus and the electrons. The opposing forces balance each other with a slight shift between the center of masses of the nucleus and the electron cloud, resulting in a polarized atom. On the other hand, a few molecules, like water,...
434
Continuous Charge Distributions
6.9K
Imagine a bucket of water. It contains many molecules, of the order of 1026 molecules. Thus, although it contains discrete elements (molecules) at the microscopic level, macroscopically, it can be considered continuous. Small volume elements of water, infinitesimal compared to the bulk of the bucket's volume, still contain many molecules. Under this framework, quantized matter is approximated as continuous for practical purposes.
The electric charge can also be subjected to an analogical...
The electric charge can also be subjected to an analogical...
6.9K
Equipotential Surfaces and Conductors
3.5K
For a conductor in which all charges are at rest, the conductor's surface is equipotential. The electric field is always perpendicular to equipotential surfaces. Therefore, in a conductor with static charges, the electric field just outside the conductor is always perpendicular to the conductor's surface. Any tangential component of the electric field will cause charges to move inside the conductor, which will violate the electrostatic nature of the system. In an electrostatic...
3.5K
Electric Field of a Charged Disk
2.2K
The simplest case of a surface charge distribution is the uniformly charged disk. Calculating its electric field also helps us calculate the electric field of a large plane of charge.
The system's symmetry is in the cylindrical directions across the plane of the charge. As a result, the electric fields created by various surface charge elements nullify each other in the direction parallel to the surface. Thereby, the resulting electric field is perpendicular to the plane. Since the disk is...
The system's symmetry is in the cylindrical directions across the plane of the charge. As a result, the electric fields created by various surface charge elements nullify each other in the direction parallel to the surface. Thereby, the resulting electric field is perpendicular to the plane. Since the disk is...
2.2K
Charge on a Conductor
4.5K
An interesting property of a conductor in static equilibrium is that extra charges on the conductor end up on its outer surface, regardless of where they originate. Consider a hollow metallic conductor with a uniform surface charge density. Since the conductor itself is in electrostatic equilibrium, there should not be any electric field inside the conductor. Now, assume a Gaussian surface enclosing the hollow portion. Applying Gauss's law, the inner surface of the hollow conductor will not...
4.5K
Electric Field at the Surface of a Conductor
4.7K
Consider a conductor in electrostatic equilibrium. The net electric field inside a conductor vanishes, and extra charges on the conductor reside on its outer surface, regardless of where they originate.
In the 19th century, Michael Faraday conducted the famous ice pail experiment to prove that the charges always reside on the surface of a conductor. The experimental set-up consists of a conducting uncharged container mounted on an insulating stand. The outer surface of the container is...
In the 19th century, Michael Faraday conducted the famous ice pail experiment to prove that the charges always reside on the surface of a conductor. The experimental set-up consists of a conducting uncharged container mounted on an insulating stand. The outer surface of the container is...
4.7K

