Jove
Visualize
Contact Us
JoVE
x logofacebook logolinkedin logoyoutube logo
ABOUT JoVE
OverviewLeadershipBlogJoVE Help Center
AUTHORS
Publishing ProcessEditorial BoardScope & PoliciesPeer ReviewFAQSubmit
LIBRARIANS
TestimonialsSubscriptionsAccessResourcesLibrary Advisory BoardFAQ
RESEARCH
JoVE JournalMethods CollectionsJoVE Encyclopedia of ExperimentsArchive
EDUCATION
JoVE CoreJoVE BusinessJoVE Science EducationJoVE Lab ManualFaculty Resource CenterFaculty Site
Terms & Conditions of Use
Privacy Policy
Policies

Related Concept Videos

Scaling01:26

Scaling

In designing and analyzing filters, resonant circuits, or circuit analysis at large, working with standard element values like 1 ohm, 1 henry, or 1 farad can be convenient before scaling these values to more realistic figures. This approach is widely utilized by not employing realistic element values in numerous examples and problems; it simplifies mastering circuit analysis through convenient component values. The complexity of calculations is thereby reduced, with the understanding that...
The Clausius–Clapeyron Equation01:29

The Clausius–Clapeyron Equation

The Clausius-Clapeyron equation is a fundamental principle in physical chemistry and thermodynamics that describes the relationship between a substance's vapor pressure and temperature. Named after Rudolf Clausius and Benoît Paul Émile Clapeyron, the equation is integral in predicting a substance's behavior under different temperature conditions.The Clausius-Clapeyron equation allows us to calculate how the pressure at which a liquid boils (its vapor pressure) changes as the temperature changes.
Euler's Equations of Motion01:28

Euler's Equations of Motion

In fluid mechanics, shear stresses arise from viscosity, which represents a fluid's internal resistance to deformation. For low-viscosity fluids, like water, these stresses are minimal, simplifying flow analysis by allowing the fluid to be treated as inviscid, or frictionless. In an inviscid fluid, shear stresses are absent, leaving only normal stresses, which act perpendicularly to fluid elements. Notably, pressure — defined as the negative of the normal stress — remains uniform across...
Navier–Stokes Equations01:28

Navier–Stokes Equations

For incompressible Newtonian fluids, where density remains constant, stresses show a linear relationship with the deformation rate, defined by normal and shear stresses. Normal stresses depend on the pressure exerted on the fluid and the rate of deformation in specific directions, which determines how fluid flows under varying pressures. Shear stresses, on the other hand, act tangentially across fluid layers. They explain how adjacent fluid layers slide relative to one another, connecting...
Modeling and Similitude01:12

Modeling and Similitude

Scaled modeling is a fundamental technique in engineering, enabling the study of large and complex systems by creating smaller, manageable replicas that recreate critical characteristics of the original. In hydrology and civil infrastructure, for example, scaled models of dams help analyze water flow, turbulence, and pressure. This method allows for accurate predictions of real-world behavior within a controlled environment, significantly reducing the cost and time involved in full-scale...
Clausius-Clapeyron Equation02:35

Clausius-Clapeyron Equation

The equilibrium between a liquid and its vapor depends on the temperature of the system; a rise in temperature causes a corresponding rise in the vapor pressure of its liquid. The Clausius-Clapeyron equation gives the quantitative relation between a substance’s vapor pressure (P) and its temperature (T); it predicts the rate at which vapor pressure increases per unit increase in temperature.

You might also read

Related Articles

Articles linked to this work by shared authors, journal, and citation graph.

Sort by
Same author

Smoluchowski Equations for Agglomeration in Conditions of Variable Temperature and Pressure and a New Scaling of Rate Constants: Application to Nozzle-Beam Expansion.

The journal of physical chemistry. A·2015
Same author

Instrument for near infrared emission spectroscopic probing of human fingertips in vivo.

The Review of scientific instruments·2010
Same author

Application of scaling and kinetic equations to helium cluster size distributions: Homogeneous nucleation of a nearly ideal gas.

The Journal of chemical physics·2006
Same author

Drug-RNA footprinting.

Methods in enzymology·2001
Same author

Characterization of hairpin-duplex interconversion of DNA using polyacrylamide gel electrophoresis.

Biophysical chemistry·2001
Same author

Binding of human immunodeficiency virus type 1 nucleocapsid protein to psi-RNA-SL3.

Biophysical chemistry·2000

Related Experiment Video

Updated: Jul 20, 2026

An Analog Macroscopic Technique for Studying Molecular Hydrodynamic Processes in Dense Gases and Liquids
11:03

An Analog Macroscopic Technique for Studying Molecular Hydrodynamic Processes in Dense Gases and Liquids

Published on: December 4, 2017

Scaling and the Smoluchowski equations.

J Goodisman1, J Chaiken

  • 1Department of Chemistry, Syracuse University, Syracuse, New York 13244-4100, USA.

The Journal of Chemical Physics
|September 1, 2006
PubMed
Summary

This study proves how cluster size distributions evolve over time in coalescence growth models. It reveals new scaling relationships and explains population oscillations in cluster dynamics.

Area of Science:

  • Physical Chemistry
  • Chemical Engineering
  • Materials Science

Background:

  • The Smoluchowski equations model cluster formation via coalescence, assuming only growth and second-order reaction rates.
  • These equations do not account for cluster breakup, a crucial process in many real-world systems.
  • Scaling of rate constants K(jk) is essential for simplifying the analysis of cluster size distributions.

Purpose of the Study:

  • To rigorously prove the asymptotic behavior of cluster size distributions for large clusters under scaling rate constants.
  • To investigate the origins of odd-even population oscillations observed for small clusters.
  • To determine the appropriate scaling exponents (mu, nu) for cluster formation from monomers via reactive collisions.

Main Methods:

More Related Videos

Analyzing Mixing Inhomogeneity in a Microfluidic Device by Microscale Schlieren Technique
10:12

Analyzing Mixing Inhomogeneity in a Microfluidic Device by Microscale Schlieren Technique

Published on: June 12, 2015

Visually Based Characterization of the Incipient Particle Motion in Regular Substrates: From Laminar to Turbulent Conditions
11:51

Visually Based Characterization of the Incipient Particle Motion in Regular Substrates: From Laminar to Turbulent Conditions

Published on: February 22, 2018

Related Experiment Videos

Last Updated: Jul 20, 2026

An Analog Macroscopic Technique for Studying Molecular Hydrodynamic Processes in Dense Gases and Liquids
11:03

An Analog Macroscopic Technique for Studying Molecular Hydrodynamic Processes in Dense Gases and Liquids

Published on: December 4, 2017

Analyzing Mixing Inhomogeneity in a Microfluidic Device by Microscale Schlieren Technique
10:12

Analyzing Mixing Inhomogeneity in a Microfluidic Device by Microscale Schlieren Technique

Published on: June 12, 2015

Visually Based Characterization of the Incipient Particle Motion in Regular Substrates: From Laminar to Turbulent Conditions
11:51

Visually Based Characterization of the Incipient Particle Motion in Regular Substrates: From Laminar to Turbulent Conditions

Published on: February 22, 2018

  • Mathematical derivation and proof of the asymptotic solution for k-mer number density.
  • Analysis of cluster velocity distributions based on collision dynamics and momentum conservation.
  • Comparison of derived scaling exponents with those from ballistic and diffusive models.
  • Main Results:

    • A transparent proof is provided for the exponential decay of large k-mer populations (Ak(a)e(-bk)).
    • The parameter 'a' is shown to be -(mu+nu), and 'b' depends linearly on time.
    • Direct calculation reveals cluster velocities proportional to m(k)(-0.577) for nascent distributions, yielding mu+nu = 0.090.

    Conclusions:

    • The derived scaling exponent (mu+nu = 0.090) is intermediate between ballistic and diffusive models, offering a more realistic description for certain systems.
    • The findings provide a theoretical basis for understanding experimental observations of cluster dynamics, including negative scaling exponents.
    • The study clarifies the relationship between collision mechanics, scaling laws, and the resulting cluster size distributions.