Principles of Chemistry CHEM 101 Lecture 7 PDF

Summary

This document covers lecture 7 of Principles of Chemistry CHEM 101, Fall 2024, at LUMS. It delves into wave functions, demonstrating calculations for orbitals like 1s, 2s, and 3s, outlining the radial distribution function (RDF) for different electronic states.

Full Transcript

Principles of Chemistry CHEM 101 Lecture 7 1 Rn,l (r) Wave function for 1s orbital of H  1s (r) 𝑟 R1,0 (r) = 𝝍𝟏𝒔 (𝑟) = 𝑁1𝑠 exp...

Principles of Chemistry CHEM 101 Lecture 7 1 Rn,l (r) Wave function for 1s orbital of H  1s (r) 𝑟 R1,0 (r) = 𝝍𝟏𝒔 (𝑟) = 𝑁1𝑠 exp − 𝑎0  (r) = N e – r/a0 R1,0 (r) = 1s 1s 1s (r) = N1s e – 0/a0 r=0 1s 2s  (r) = N e – 0 1s 1s 1s (r) = N1s 1 0 a0 2a0 3a0 r  1s (r) = N1s e – 0/a0 a r = a0 1s (r) = N1s e – 1 1s (r) = N1s 0.368 1s (r) = N1s 0.135 r = 2 a0 1s (r) = N1s 0.00674 r = 5 a0 1s (r) = N1s 0.0497 r = 3 a0 1s (r) = N1s 0.000045 r = 10 a0 2 Rn,l (r) 1s (r) = N1s e – r/a0 Wave function for 2s orbital of H R2,0 (r) = 2s (r) = N2s (2 – r/a0 ) e -r/2a0 2s (r) = N2s (2 – 3a0/a0 ) e – 3a0/2a0 r = 3 a0  (r) = N (2 – 3) e-1.5 2s 2s r = 10 a0 r=0 2s (r) = N2s (2 – 0/a0 ) e – 0/2a0 2s (r) = N2s (– 1) 0.223 = – N2s 0.223 2s (r) = – N2s 0.054 2s (r) = N2s (2 – 0 ) e-0 2s (r) = N2s (2 – 4a0/a0 ) e – 4a0/2a0 r = 4 a0 2s (r) = N2s (2) 1 = N2s 2  (r) = N (2 – 4) e-2 2s 2s 2s (r) = N2s (2 – a0/a0 ) e – a0/2a0 r = a0 2s (r) = N2s (– 2) 0.135 = – N2s 0.27 2s  (r) = N (2 – 1 ) e-0.5 2s (r) = N2s (2 – 5a0/a0 ) e – 5a0/2a0 Radial node 2s 2s r = 5 a0  2s (r) = N2s (1 ) 0.606 = N2s 0.606  (r) = N (2 – 5) e-2.5 r = 2a0 2s 2s 2s (r) = N2s (2 – 2a0/a0 ) e – 2a0/2a0 r = 2 a0 2s (r) = N2s (– 3) 0.082 = – N2s 0.246 0 r  (r) = N (2 – 2 ) e-1 2s 2s 2s (r) = N2s (2 – 8a0/a0 ) e – 8a0/2a0 r = 8 a0 2s (r) = N2s (0 ) 0.369 = 0 2s (r) = N2s (2 – 8) e-4 r = 4a0 2s (r) = N2s (– 6) 0.0183 = – N2s 0.101 3 Rn,l (r) Wave function for 2s orbital of H Wave function for 1s orbital of H  1s (r) -r/2a0 R2,0 (r) = 2s (r) = N2s (2 – r/a0 ) e 2s 2s (r) = N2s 2 r=0 2s (r) = N2s 0.606 r = a0 2s (r) = 0 r = 2 a0 (r) 2s (r) = – N2s 0.22 r = 3 a0 2s (r) = – N2s 0.27 r = 4 a0 2s (r) = – N2s 0.246 r = 5 a0 Radial Node 0 a0 2a0 3a0 r 2s (r) = – N2s 0.101 r = 8 a0 r = 2a0 2s (r) = – N2s 0.054 r = 10 a0 0 r r = 4a0 1s 2s 4 Rn,l (r) Wave function for 3s orbital of H  3s = N3s {27 –18( r/a0 )+2 ( r/a0 )2} e-r/3a0 3s (r) Radial Node Radial Node r 5 Rn,l (r) Radial part of the wavefunctions   1s 2s  3s 0 r 0 r 0 r No radial node 1 radial node 2 radial node 6 Rn,l (r) 2s (r) = N2s (2 – r/a0 ) e-r/2a0  2p = N2p (10) e-5 r = 10 a0 Wave function for 2p orbital of H  2p = N2p (10) 0.007 = N2p0.07 R2,1 (r) =  2p = N2p (r/a0 ) e -r/2a0  2p = N2p (4) e-2 r = 4 a0  2p = N2p (4) 0.135 = N2p0.54  2p = N2p (11) e-5.5 r = 11 a0  2p = N2p (0/a0 ) e -0/2a0 r=0  2p = N2p (11) 0.004 = N2p0.04  2p = N2p (5) e-2.5 r = 5 a0  2p = N2p (0) 1 = 0  2p = N2p (12) e-6 r = 12 a0  2p = N2p (5) 0.082 = N2p0.41  2p = N2p (a0/a0 ) e-a0/2a0 r = a0  2p = N2p (12) 0.002 = N2p0.02  2p = N2p (6) e-3 r = 6 a0  2p = N2p (1) e-0.5  2p = 0 r=0  2p = N2p (6) 0.05 = N2p0.3  2p = N2p0.606 r = a0  2p = N2p0.756  2p = N2p (1) 0.606 = N2p0.606  2p = N2p (7) e-3.5 r = 7 a0  2p = N2p0.669 r = 2a0 r = 3a0 r = 2 a0  2p = N2p (7) 0.03 = N2p0.21  2p = N2p0.54 r = 4a0  2p = N2p (2a0/a0) e-1  2p = N2p0.41 r = 5a0  2p = N2p (2) 0.378 = N2p0.756  2p = N2p (8) e-4 r = 8 a0  2p = N2p0.3 r = 6a0  2p = N2p0.21 r = 7a0  2p = N2p (8) 0.018 = N2p0.14  2p = N2p0.14 r = 8a0  2p = N2p (3a0/a0) e-1.5 r = 3 a0  2p = N2p0.09 r = 9a0  2p = N2p (9) e-4.5 r = 9 a0  2p = N2p0.07 r = 10a0  2p = N2p (3) 0.223 = N2p0.669  2p = N2p0.04 r = 11a0  2p = N2p (9) 0.011 = N2p0.09  2p = N2p0.02 r = 12a0 Rn,l (r) Wave function for 2p orbital of H R2,1 (r) =  2p = N2p (r/a0 ) e -r/2a0  2p = 0 r=0  2p = N2p0.606 r = a0 (r) 2p  2p = N2p0.756 r = 2a0  2p = N2p0.669 r = 3a0  2p = N2p0.54 r = 4a0  2p = N2p0.41 r = 5a0  2p = N2p0.3 r = 6a0  2p = N2p0.21 r = 7a0 r  2p = N2p0.14 r = 8a0  2p = N2p0.09 r = 9a0  2p = N2p0.07 r = 10a0 Angular Node, nodal plane  2p = N2p0.04 r = 11a0  2p = N2p0.02 r = 12a0 8 Rn,l (r) (r) Wave function for 3p orbital of H 2p R3,1 (r) = 3p = N3p {6(r/a0)– (r/a0)2 } e-r/3a0 r 3p Angular Node, nodal plane (r) r Angular Node, nodal plane Radial Node 9 Rn,l (r) Radial part of the wavefunctions (r) 1s (r) 2s (r) 3s 0 r 0 r 0 r (r) 2p (r) 3p 0 r 0 r 10 Probability of finding the electron in a thin shell of radius r and thickness  r. r Area of a sphere of radius r = 4 r2 Volume of a shell of radius r and thickness r = 4 r2   r =  V Probability of electron in volume V = [1s(r)]2  4 r2   r Radial distribution function (RDF) P1s (r) = [1s(r)]2  V RDF P1s (r) = [1s(r)]2  4 r2 If  r is kept constant, then RDF 1. [1𝑠 (𝑟)]2 depends only on two terms: 2. 𝑟2 Radial distribution Functions (RDF) of ns orbitals 1s (r) = [R1s (r)] 2s (r) = [R2s (r)] P1s (r) = [R1s (r)]2  r2 P2s (r) = [R2s (r)]2  r2 1s 2s rmp = a0 P2s (r)  RDF r a0 2a0 3a0 r [1s (r)]2 Radial node r2 r2 r2 r a0 2a0 3a0 r 12 Radial distribution Functions (RDF) of ns orbitals 3s (r) = [R3s (r)] P3s (r) = [R3s (r)]2  r2 P2s (r) P3s (r) 3s   r r Radial node 2 Radial nodes [1s (r)]2 P1s (r) = [1s (r)]2  r2 RDF r2 r2 r2 r r a0 2a0 3a0 r 13 a0 2a0 3a0 Radial distribution Functions (RDF) of 1s, 2s, and 3s orbitals rmp = a0 1s rmp = ~5a0 P(r) rmp= ~11a0 2s 3s r 14 Radial distribution Functions (RDF) of 2p and 3p orbitals 2p (r) = [R2p (r)] 3p (r) = [R2p (r)] P2p (r) = [R2p (r)]2  r2 P3p (r) = [R2p (r)]2  r2 2p 3p P3p (r)   P2p (r) r r nodes node 15 Radial distribution Functions (RDF) of 1s, 2s and 2p orbitals rmp = a0 1s P(r) rmp = ~4a0 2p 2s rmp = ~5a0 r 16

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