اللزوجة المعتمدة على الزمن: اللزوجة والثبات

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.

انكماش اللانثانيدات هو التناقص المستمر في نصف القطر الذري والأيوني لعناصر اللانثانيدات (من اللانثانوم إلى اللوتيتيوم) مع تزايد العدد الذري. يحدث هذا التأثير بسبب ضعف حجب الشحنة النووية بواسطة إلكترونات 4f. وينتج عن ذلك أن تكون عناصر الدورة السادسة التي تلي اللانثانيدات صغيرة بشكل غير متوقع، على غرار نظيراتها من الدورة الخامسة.

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).

الترقق القصي، أو شبه اللدونة، هو سلوك غير نيوتوني، حيث تنخفض لزوجة السائل مع تزايد معدل إجهاد القص. تُظهر العديد من المواد الشائعة، مثل الكاتشب والطلاء، هذه الخاصية. تكون هذه المواد سميكة في حالة السكون، لكنها تتدفق بسهولة أكبر عند رجها أو تحريكها أو فردها. وغالبًا ما يُمثل ذلك بعلاقة قانون أوستوالد-دي فالي للقوة.

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].

الصمام الثنائي الباعث للضوء عبارة عن وصلة pn شبه موصلة. عند تطبيق جهد أمامي مناسب، تُحقن الإلكترونات من الجانب n والفجوات من الجانب p في منطقة الاستنزاف. وعندما تتحد هذه الإلكترونات والفجوات، تُطلق الطاقة. في أشباه الموصلات ذات فجوة النطاق المباشرة، تُبعث هذه الطاقة بكفاءة على شكل فوتونات ضوئية، وهي عملية تُعرف باسم التألق الكهربائي.

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.