pH

Autocatalysis is a chemical reaction where one of the reaction products is also a catalyst for the same or a coupled reaction. This creates a positive feedback loop, leading to an accelerating reaction rate. The rate of reaction is initially slow but increases as the concentration of the product (catalyst) builds up, often resulting in sigmoidal (S-shaped) kinetic curves.

The Landé g-factor (\(g_J\)) is a dimensionless proportionality constant that relates an atom's total magnetic moment to its total angular momentum in the weak-field limit. It is crucial for quantitatively explaining the anomalous Zeeman effect. Its value is given by the formula: \(g_J = 1 + \frac{J(J+1) + S(S+1) - L(L+1)}{2J(J+1)}\), where L, S, and J are the quantum numbers.

All quantum entities, such as photons and electrons, exhibit both particle and wave properties. Depending on the experimental setup, they can behave like a localized particle or a distributed wave. The de Broglie hypothesis states that any particle with momentum \(p\) has an associated wavelength \(\lambda = h/p\), where \(h\) is Planck's constant.

The lanthanide contraction is the steady decrease in the atomic and ionic radii of the lanthanide elements (lanthanum to lutetium) with increasing atomic number. This effect is caused by the poor shielding of the nuclear charge by the 4f electrons. It results in the 6th-period elements following the lanthanides being unexpectedly small, similar to their 5th-period counterparts.

Quantum statistics modifies classical statistical mechanics to account for the indistinguishability of identical particles. It splits into two types: Fermi-Dirac statistics for fermions (half-integer spin particles like electrons), which obey the Pauli exclusion principle, and Bose-Einstein statistics for bosons (integer spin particles like photons), which can occupy the same quantum state. This distinction is crucial at low temperatures and high densities.

Thixotropy and rheopexy describe time-dependent changes in viscosity. A thixotropic fluid's viscosity decreases over time under constant shear stress (e.g., yogurt becomes runnier when stirred). A rheopectic (or anti-thixotropic) fluid's viscosity increases over time under constant shear (e.g., some lubricants). These effects are reversible; the fluid returns to its original state after a period of rest.

A Bingham plastic is a viscoplastic material that behaves as a rigid body at low stresses but flows as a viscous fluid at high stress. It is characterized by a yield stress, \(\tau_0\), which is the minimum shear stress required to initiate flow. Below this threshold, it does not deform. Common examples include toothpaste, mayonnaise, and clay slurries.

Shear-thinning, or pseudoplasticity, is a non-Newtonian behavior where a fluid's viscosity decreases with an increasing rate of shear stress. Many common substances, like ketchup or paint, exhibit this property. At rest, they are thick, but they flow more easily when shaken, stirred, or spread. This is often modeled by the Ostwald–de Waele power-law relationship.

This is a fundamental equation in quantum mechanics that describes how the quantum state of a physical system changes over time. It is a linear partial differential equation for the wavefunction, \(\Psi(x, t)\). The time-dependent version is \(i\hbar\frac{\partial}{\partial t}\Psi = \hat{H}\Psi\), where \(\hat{H}\) is the Hamiltonian operator, representing the total energy of the system.

In quantum mechanics, momentum is an observable represented by a vector operator. In the position basis, the momentum operator is given by \(\hat{\vec{p}} = -i\hbar\nabla\), where \(\hbar\) is the reduced Planck constant and \(\nabla\) is the gradient operator. The conservation of momentum corresponds to the fact that the Hamiltonian operator commutes with the momentum operator, \([\hat{H}, \hat{\vec{p}}] = 0\), for a system with translational symmetry.

It is impossible to simultaneously know with perfect accuracy certain pairs of complementary physical properties of a particle. The most common example is the position \(x\) and momentum \(p\). The principle states that the product of their uncertainties, \(\Delta x\) and \(\Delta p\), must be greater than or equal to a specific value: \(\Delta x \Delta p \ge \frac{\hbar}{2}\).