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Newton's law of gravitation resembles Coulomb's law of electrical forces, which is used to calculate the magnitude of the electrical force arising between two charged bodies. Both are inverse-square laws, where force is inversely proportional to the square of the distance between the bodies. Coulomb's law has charge in place of mass and a ...
The potential is monotonically increasing in r and it is negative, implying the force is attractive. In the SI system, the unit of the Yukawa potential is the inverse meter . The Coulomb potential of electromagnetism is an example of a Yukawa potential with the e − α m r {\displaystyle e^{-\alpha mr}} factor equal to 1, everywhere.
Under these conditions an attractive force appears, whose magnitude depends on the voltage and the specific materials involved. The attractive force is much larger than would be produced by Coulombic attraction. The effect is named after Danish engineers F. A. Johnsen and K. Rahbek, the first to investigate the effect at length.
The SI unit of force is the newton (symbol N), which is the force required to accelerate a one kilogram mass at a rate of one meter per second squared, or kg·m·s −2.The corresponding CGS unit is the dyne, the force required to accelerate a one gram mass by one centimeter per second squared, or g·cm·s −2. A newton is thus equal to ...
A depletion force is an effective attractive force that arises between large colloidal particles that are suspended in a dilute solution of depletants, which are smaller solutes that are preferentially excluded from the vicinity of the large particles.
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ε 0 is the permittivity of free space; q 1, q 2 are the charges of the interacting particles; r is the interaction radius. A positive value of U is due to a repulsive force, so interacting particles are at higher energy levels as they get closer. A negative potential energy indicates a bound state (due to an attractive force).
On the PB level, however, attractive three-body forces are present. [11] The interaction free energy between three objects 1, 2, and 3 can be expressed as = + + + where F ij are the pair free energies and ΔF 123 is the non-additive three-body contribution. These three-body contributions were found to be attractive on the PB level, meaning that ...