Search
- Filter Results
- Location
- Classification
- Include attachments
- https://chem.libretexts.org/Bookshelves/Inorganic_Chemistry/Introduction_to_Solid_State_Chemistry/05%3A_CHEM_ATLASes
- https://chem.libretexts.org/Bookshelves/Inorganic_Chemistry/Principles_of_Inorganic_Chemistry_II_(Nocera)/02%3A_Assignments/2.02%3A_New_PageConsider the three center bond of the Al 2 (µ-CH 3 ) 2 unit in “trimethyl aluminum” which exists as the dimer [Al(CH 3 ) 3 ] 2 in the gas phase and nonpolar solvents. 1,3,5-hexatriene and benzene are ...Consider the three center bond of the Al 2 (µ-CH 3 ) 2 unit in “trimethyl aluminum” which exists as the dimer [Al(CH 3 ) 3 ] 2 in the gas phase and nonpolar solvents. 1,3,5-hexatriene and benzene are limiting cases for a more general molecular orbital system in which the interaction energy for the terminal orbitals, β 1 ,6 , is finite and not equal to the interaction energy between adjacent orbitals.
- https://chem.libretexts.org/Bookshelves/Inorganic_Chemistry/Introduction_to_Solid_State_Chemistry/02%3A_Assessments/2.07%3A_Self-Assessment-_Solid_Solutions\(\begin{array}{ll}\mathrm{T}_{\mathrm{M}} \mathrm{Ag}: & 960^{\circ} \mathrm{C} \\ \mathrm{T}_{\mathrm{M}} \mathrm{Cu}: & 1080^{\circ} \mathrm{C} \\ \mathrm{T}_{\mathrm{E}} \text { (Eutectic) } & 780...TMAg:960∘CTMCu:1080∘CTE (Eutectic) 780∘C:α[9wt.%Cu];β[92wt.%Cu]; Eutectic comp. 28wt.%Cu400∘C:α[1wt.%Cu];β[100wt.%Cu]
- https://chem.libretexts.org/Bookshelves/Physical_and_Theoretical_Chemistry_Textbook_Maps/Non-Equilibrium_Statistical_Mechanics_(Cao)/04%3A_Time_Correlation_Functions/4.02%3A_Projection_Operator_Method\[\begin{aligned} \frac{d v}{d t} &=-\int_{0}^{t} \gamma(t-\tau) v(\tau) d \tau+\frac{f(t)}{m} \\ \frac{d v}{d t} v(0) &=-\int_{0}^{t} \gamma(t-\tau) v(\tau) v(0) d \tau+\frac{f(t)}{m} v(0) \\ \left\l...dvdt=−∫t0γ(t−τ)v(τ)dτ+f(t)mdvdtv(0)=−∫t0γ(t−τ)v(τ)v(0)dτ+f(t)mv(0)⟨dvdtv(0)⟩=−∫t0γ(t−τ)⟨v(τ)v(0)⟩dτ+v(0)m⟨f(t)⟩dC(t)dt=−∫t0γ(t−τ)C(τ)dτ
- https://chem.libretexts.org/Bookshelves/Physical_and_Theoretical_Chemistry_Textbook_Maps/Non-Equilibrium_Statistical_Mechanics_(Cao)/02%3A_Non-equilibrium_Thermodynamics/2.03%3A_Linear_Response_Theory_and_CausalityThe concept of linear response was introduced in section 2.1. Here, we explore further how the linear response of a system is quantified by considering the important relations regularly invoked by pra...The concept of linear response was introduced in section 2.1. Here, we explore further how the linear response of a system is quantified by considering the important relations regularly invoked by practitioners of linear response theory.
- https://chem.libretexts.org/Bookshelves/Inorganic_Chemistry/Introduction_to_Solid_State_Chemistry/06%3A_Recitations/6.01%3A_Balancing_Reactions_Yield_and_Limiting_ReagentsThe number of each type of atom in the reactants must equal the number of each type of atom in the products a) To balance the reaction, we can start by looking at the Cl atoms: we need to...The number of each type of atom in the reactants must equal the number of each type of atom in the products a) To balance the reaction, we can start by looking at the Cl atoms: we need to double the MgCl2 on the right to equal the left. The balanced reaction tells us we get two moles of MgCl2 and 1 mole of Ti per mole of Mg we react, so the yield is
- https://chem.libretexts.org/Ancillary_Materials/Laboratory_Experiments/Wet_Lab_Experiments/Organic_Chemistry_Labs/Intermediate_Chemical_Experimentation/03%3A_BiochemistryProtein Data Bank viewer software can be used to view .pdb protein data bank files. PDB Files: 1GSO.pdb, 1GSOsubs.pdb, 1IOV.pdb Rasmol Protein Explorer Front Door
- https://chem.libretexts.org/Bookshelves/Inorganic_Chemistry/Principles_of_Inorganic_Chemistry_II_(Nocera)/02%3A_Assignments/2.01%3A_New_PageConsider the trigonal planar molecule, BF 3 . Use the three fluorine atoms as an arbitrary basis set to describe the matrix representation for each of the operations in the point group (relying on the...Consider the trigonal planar molecule, BF 3 . Use the three fluorine atoms as an arbitrary basis set to describe the matrix representation for each of the operations in the point group (relying on the methods employed above, solve the appropriate eigenvalue problem). Construct the similarity transformation matrix θ from the eigenvectors and determine θ -1 . For the case where the eigenvectors are complex, take linear combinations to yield eigenvectors in real space.
- https://chem.libretexts.org/Bookshelves/Physical_and_Theoretical_Chemistry_Textbook_Maps/Non-Equilibrium_Statistical_Mechanics_(Cao)/00%3A_Front_Matter/02%3A_InfoPageThe LibreTexts libraries are Powered by MindTouch ® and are supported by the Department of Education Open Textbook Pilot Project, the UC Davis Office of the Provost, the UC Davis Library, the Californ...The LibreTexts libraries are Powered by MindTouch ® and are supported by the Department of Education Open Textbook Pilot Project, the UC Davis Office of the Provost, the UC Davis Library, the California State University Affordable Learning Solutions Program, and Merlot.
- https://chem.libretexts.org/Bookshelves/Inorganic_Chemistry/Principles_of_Inorganic_Chemistry_II_(Nocera)/02%3A_Assignments/2.04%3A_New_PageThe spectroscopy of Cr(III) in the solid state is the underpinning for the invention in the 1960’s of the first solid state laser, the ruby laser.
- https://chem.libretexts.org/Bookshelves/Inorganic_Chemistry/Principles_of_Inorganic_Chemistry_II_(Nocera)/01%3A_Chapters/1.11%3A_Frontier_molecular_orbitals_of_-donor_-donor_and_-acceptor_ligands&\mathrm{P}^{\mathrm{a}_{1}}\left(\sigma_{1}\right) \rightarrow 1 \cdot \overbrace{ {\mathrm{E} \sigma_{1}}}^{ \sigma_{1}}+1 \cdot \overbrace{ {\mathrm{C}_{2} \sigma_{1}} }^{\sigma_{2}}+1 \cdot \overb...&\mathrm{P}^{\mathrm{a}_{1}}\left(\sigma_{1}\right) \rightarrow 1 \cdot \overbrace{ {\mathrm{E} \sigma_{1}}}^{ \sigma_{1}}+1 \cdot \overbrace{ {\mathrm{C}_{2} \sigma_{1}} }^{\sigma_{2}}+1 \cdot \overbrace{ {\sigma(\mathrm{xz}) \cdot \sigma_{1}} }^{\sigma_{1}}+1 \cdot \overbrace{ {\sigma(\mathrm{yz}) \cdot \sigma_{1}} }^{\sigma_{2}} \rightarrow \psi_{\mathrm{a}_{1}}=\frac{1}{\sqrt{2}}\left(\sigma_{1}+\sigma_{2}\right)\\
