
Fick's laws of diffusion describe the movement of molecules from a higher concentration to a lower concentration region. Fick's first law predicts the flux of reactants to the substrate and the product away from the substrate, with the direction of flux being from regions of high concentration to regions of low concentration. The rate of flow of particles through an area is the flux, and it is plotted on a graph with the gradient. The flux is dependent on the steepness of the gradient and a proportionality coefficient based on the substance being measured.
| Characteristics | Values |
|---|---|
| Flux | The number of particles moving past a given region divided by the area of that region multiplied by the time interval |
| Direction of Flux | From high concentration to low concentration |
| Diffusion Coefficient | Tells you something about the system, e.g. the substance, temperature, and viscosity |
| Units of Flux | mol m-2 s-1 |
| Units of Diffusion Coefficient | m2 s |
| Units of Concentration | molecules m-3 |
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What You'll Learn

Fick's first law of diffusion
Fick's laws of diffusion describe diffusion and were first posited by Adolf Fick in 1855, inspired by the earlier experiments of Thomas Graham. Fick's first law of diffusion can be used to derive his second law, which is identical to the diffusion equation.
Fick's first law states that the movement of particles from high to low concentration (diffusive flux) is directly proportional to the particle's concentration gradient. In other words, the flux goes from regions of high concentration to regions of low concentration, with a magnitude that is proportional to the concentration gradient. This can be represented on a graph, with the flux plotted on the vertical axis and the gradient on the horizontal axis. The flux is dependent on two quantities: the steepness of the gradient and a proportionality coefficient based on the substance being measured (called the diffusion coefficient, "D").
The diffusion coefficient is a critical component of Fick's first law. It can be used to solve for the diffusion coefficient, and its value changes as the properties of the system change. For example, at higher temperatures, the diffusion coefficient is greater due to increased molecular motion. The diffusion coefficient is also related to the viscosity of the solution, with a higher diffusion coefficient corresponding to lower viscosity.
Fick's first law can be applied to various systems, including solids, liquids, and gases. However, it is essential to note that it only applies under specific conditions. For example, in the case of semiconductors, Fick's first law only applies to certain boundary conditions, such as constant source concentration diffusion or limited source concentration.
Fick's first law is also important in radiation transfer equations. However, it becomes inaccurate when the diffusion constant is low, and the radiation is limited by the speed of light rather than the material's resistance. In such cases, a flux limiter can be used.
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Flux and concentration gradient
Fick's laws of diffusion describe diffusion and were first proposed by Adolf Fick in 1855. Fick's experiments dealt with measuring the concentrations and fluxes of salt diffusing between two reservoirs through tubes of water. Fick's first law relates the diffusive flux to the gradient of concentration. It states that the flux goes from regions of high concentration to regions of low concentration, with a magnitude that is proportional to the concentration gradient. In other words, it predicts the movement of particles from high to low concentration (diffusive flux) and is directly proportional to the particle's concentration gradient.
Diffusion is the net movement of anything, including atoms, ions, molecules, and energy, generally from a region of higher concentration to a region of lower concentration. It is driven by a gradient in Gibbs free energy or chemical potential. A gradient is the change in the value of a quantity, such as concentration, pressure, or temperature, with respect to another variable, usually distance. A change in concentration over a distance is called a concentration gradient.
The direction of flux in Fick's law is from regions of high concentration to regions of low concentration. This is because diffusion always goes down the concentration gradient, in the opposite direction of the gradient. The rate of flow of particles through an area is the flux. The diffusion coefficient, denoted as 'D', is an important concept in Fick's law. It represents the diffusion coefficient with units of m^2/s. The diffusion coefficient can be used to calculate the flux and the change in concentration over time.
Fick's first law can be represented on a graph, with flux plotted on the vertical axis and the gradient on the horizontal axis. The flux depends on two quantities: the steepness of the gradient and a proportionality coefficient based on the specific substance being measured, which is the diffusion coefficient. Fick's first law is also applicable in radiation transfer equations. However, it becomes inaccurate when the diffusion constant is low, and the radiation is limited by the speed of light rather than the resistance of the material it is flowing through. In such cases, a flux limiter can be used.
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Flux and temperature
Fick's laws of diffusion describe diffusion and were first posited by Adolf Fick in 1855 based on experimental results. Fick's first law relates the diffusive flux to the gradient of concentration. It states that the flux moves from regions of high concentration to regions of low concentration, with a magnitude proportional to the concentration gradient. The law can be used to derive Fick's second law, which predicts changes in the concentration gradient over time due to diffusion.
Now, flux and temperature are closely related concepts. Heat flux, or thermal flux, refers to the rate at which heat is transferred per unit area per unit time through an object or substance. It is typically measured in watts per square meter (W/m²) and represents the flow of energy per unit area per unit time. Heat flux is a vector quantity, possessing both a direction and a magnitude. The direction of heat flux is from regions of higher temperature to lower temperature, indicating that heat always flows from a hotter area to a colder one.
The temperature gradient, which is the difference in temperature between two points or regions, influences the direction and magnitude of heat flux. A greater temperature difference results in a higher rate of heat transfer or flux. Additionally, the thermal conductivity of the material through which heat is flowing also affects the heat flux. Materials with higher thermal conductivity allow for more efficient heat transfer, resulting in a higher flux.
Fick's first law also acknowledges the influence of temperature on flux. According to the law, increasing the temperature can increase the diffusivity of particles. This means that raising the temperature can enhance the movement of particles from high to low concentration, thereby impacting the overall flux.
In summary, flux and temperature are interconnected, with temperature gradients and thermal conductivity influencing the direction and magnitude of heat flux. Fick's laws provide insights into how temperature variations can affect the flux of particles during diffusion processes.
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Flux and pressure
Fick's laws of diffusion describe diffusion and were first posited by Adolf Fick in 1855 based on experimental results. Fick's first law predicts the movement of particles from high to low concentration, with the magnitude of the movement being directly proportional to the concentration gradient. This law can be used to determine the diffusion coefficient, which is useful for identifying substances as it varies across different substances.
Fick's first law can be applied to control the diffusivity and growth of thin films of semiconductors by manipulating partial pressure gradients. The law is represented on a graph with flux plotted on the vertical axis and the concentration gradient plotted on the horizontal axis. The flux is dependent on the steepness of the gradient and a proportionality coefficient based on the substance being measured, known as the diffusion coefficient.
Now, onto the relationship between flux and pressure. Flux implies movement, and in the context of pressure, it refers to the flow rate per unit area. Pressure is force per unit area, and force is a momentum transfer rate, which can be described as momentum divided by time or pressure multiplied by the surface area. Pressure flux specifically refers to the transport of pressure, and its convergence or divergence is associated with larger-scale eddies.
In the context of Fick's law, the direction of flux is from regions of high concentration to regions of low concentration, with the magnitude of the flux being proportional to the concentration gradient. This means that the flux moves in the direction opposite to the gradient.
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Normal vs anomalous diffusion
Fick's laws of diffusion describe diffusion and were first posited by Adolf Fick in 1855 based on experimental results. Fick's first law of diffusion relates the diffusive flux to the gradient of concentration. It states that the flux goes from regions of high concentration to regions of low concentration, with a magnitude proportional to the concentration gradient. Fick's second law predicts the change in concentration gradient over time due to diffusion.
Diffusion processes that follow Fick's laws are called normal or Fickian diffusion. Fick's work was primarily focused on diffusion in fluids, as diffusion in solids was not generally considered possible at the time. However, today, Fick's laws are fundamental to our understanding of diffusion in solids, liquids, and gases.
When a diffusion process deviates from Fick's laws, it is termed non-Fickian or anomalous diffusion. Anomalous diffusion exhibits a non-linear relationship between the mean squared displacement (MSD) and time, contrasting with the linear relationship observed in typical diffusion processes like Brownian motion. Anomalous diffusion can be further classified into subdiffusion (α < 1), superdiffusion (1 < α < 2), and ballistic motion (α = 2).
Normal diffusion, described by a Gaussian probability density function, exhibits a variance that increases linearly with time. In contrast, anomalous diffusion regimes can be characterised by a slower or faster increase in variance compared to normal diffusion. For example, in superdiffusion, the variance diverges. Anomalous diffusion processes can be modelled using fractional diffusion equations, with Continuous Time Random Walk (CTRW) and fractional Brownian motion being prominent examples.
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Frequently asked questions
Fick's laws of diffusion describe the movement of molecules from a higher concentration to a lower concentration region. Fick's first law relates the diffusive flux to the gradient of concentration.
The direction of flux is from a region of high concentration to a region of low concentration.
Fick's first law can be represented by the equation:
J =-D∇φ
Where J is the diffusion flux, D is the diffusivity, and φ is the concentration.
The units of J are mol m^-2 s^-1. The units of D are m^2/s. The units of φ are molecules per m^3.
The negative sign in the equation indicates that the concentration gradient is negative. This is because diffusion always occurs in the direction opposite to the concentration gradient, i.e., from high to low concentration.






































