时间依赖性粘度：触变性和流变性

pH is formally defined as the negative decimal logarithm of the hydrogen ion activity, [latex]a_{H^+}[/latex]. The formula is [latex]pH = -\log_{10}(a_{H^+})[/latex]. Activity is the effective concentration of hydrogen ions, accounting for intermolecular forces, and is dimensionless. For dilute solutions, activity is approximately equal to the molar concentration of [latex]H^+[/latex] ions, simplifying the calculation.

镧系收缩是指镧系元素（从镧到镥）的原子半径和离子半径随着原子序数的增加而逐渐减小的现象。这种效应是由于4f电子对核电荷的屏蔽作用较弱造成的。这导致镧系元素之后的第六周期元素意外地小，与第五周期元素相似。

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.

A quantum mechanical phenomenon where a wavefunction can propagate through a potential energy barrier. Classically, a particle lacking sufficient energy to surmount a barrier would be reflected. However, due to the wave-like nature of particles, there is a non-zero probability that the particle can appear on the other side of the barrier, effectively 'tunneling' through it.

A non-Newtonian fluid is one whose viscosity changes under an applied shear stress. Unlike a Newtonian fluid where viscosity is constant, its flow properties are not described by a linear relationship between shear stress ([latex]\tau[/latex]) and shear rate ([latex]\dot{\gamma}[/latex]). This dependency can manifest as shear-thinning (viscosity decreases with stress) or shear-thickening (viscosity increases with stress).

剪切稀化，或称假塑性，是一种非牛顿行为，指流体的粘度随剪切应力的增加而降低。许多常见物质，例如番茄酱或油漆，都表现出这种特性。静止状态下，它们很稠，但在摇晃、搅拌或摊开时更容易流动。这通常用奥斯特瓦尔德-德瓦勒幂律关系来描述。

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, [latex]\Psi(x, t)[/latex]. The time-dependent version is [latex]i\hbar\frac{\partial}{\partial t}\Psi = \hat{H}\Psi[/latex], where [latex]\hat{H}[/latex] 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 [latex]\hat{\vec{p}} = -i\hbar\nabla[/latex], where [latex]\hbar[/latex] is the reduced Planck constant and [latex]\nabla[/latex] is the gradient operator. The conservation of momentum corresponds to the fact that the Hamiltonian operator commutes with the momentum operator, [latex][\hat{H}, \hat{\vec{p}}] = 0[/latex], 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 [latex]x[/latex] and momentum [latex]p[/latex]. The principle states that the product of their uncertainties, [latex]\Delta x[/latex] and [latex]\Delta p[/latex], must be greater than or equal to a specific value: [latex]\Delta x \Delta p \ge \frac{\hbar}{2}[/latex].

发光二极管是一种半导体PN结。当施加合适的正向电压时，n区的电子和p区的空穴被注入到耗尽区。当它们复合时，会释放能量。在直接带隙半导体中，这种能量会高效地以光子的形式释放出来，这一过程称为电致发光。

Electrochemical potential, [latex]\bar{\mu}_i[/latex], quantifies the total energy of a charged species `i` in a system. It combines the chemical potential, [latex]\mu_i[/latex], which accounts for concentration and intrinsic properties, with the electrostatic potential energy, [latex]z_i F \phi[/latex]. The formula is [latex]\bar{\mu}_i = \mu_i + z_i F \phi[/latex], where [latex]z_i[/latex] is the ion's charge, [latex]F[/latex] is the Faraday constant, and [latex]phi[/latex] is the local electric potential.