Electronics Labs - Digital Electronics
Zhenyu Ye
14-Nov-16 1
The Art of Electronics by Horowitz and Hill β Chapter 8
Boolean AlgebraBoolean algebra is the branch of algebra in which the values of the variables are the truth values:true and false, usually denoted as 1 and 0. Instead of elementary algebra where the values of the variables are numbers, and the main operations are addition and multiplication, the basic operations of Boolean algebra are n conjunction and denoted as π΄ β§ π΅, π΄ $ π΅n disjunction or denoted as π΄ β¨ π΅, π΄+ π΅n negation not denoted as Β¬π, οΏ½Μ οΏ½
October 24, 2016 Digit Electronics, Zhenyu Ye 4
Boolean Algebra βTruth Table
October 24, 2016 Digit Electronics, Zhenyu Ye 5
x y π± $ π π + π0 0 0 01 0 0 10 1 0 11 1 1 1
π± π-0 11 0
Boolean Algebra β Secondary Ops.
NAND n π₯ $ π¦ = οΏ½Μ οΏ½ + π¦1
NORn π₯ + π¦ = οΏ½Μ οΏ½ $ π¦1
October 24, 2016 Digit Electronics, Zhenyu Ye 6
x y π $ π π- + π-0 0 1 11 0 1 10 1 1 11 1 0 0
x y π + π π- $ π-0 0 1 11 0 0 00 1 0 01 1 0 0
Boolean Algebra β Secondary Ops.
n Exclusive OR (XOR)πβ π = (π + π) $ (π $ π)
October 24, 2016 Digit Electronics, Zhenyu Ye 7
x y πβ π (π + π) (π $ π)0 0 0 0 11 0 1 1 10 1 1 1 11 1 0 1 0
Boolean Algebra β De Morganβs Laws
n Associativity of OR x + π¦ + π§ = π₯ + π¦ + π§n Associativity of AND x $ π¦ $ π§ = π₯ $ π¦ $ π§n Commutativity of OR x + π¦ = π¦ + π₯n Commutativity of AND x $ π¦ = π¦ $ π₯n Distributivity of AND over OR
x $ π¦ + π§ = π₯ $ π¦ + (π₯ $ π§)n Distributivity of OR over AND
x+ π¦ $ π§ = π₯ + π¦ $ (π₯ + π§)
October 24, 2016 Digit Electronics, Zhenyu Ye 8
Brownian Motionn Brownian Motion is the random motion of particles
suspended in a fluid (a liquid or a gas) resulting fromtheir collision with the fast-moving atoms ormolecules in the gas or liquid.
n https://upload.wikimedia.org/wikipedia/commons/6/6d/Translational_motion.gif
n https://upload.wikimedia.org/wikipedia/commons/5/51/Brownianmotion5particles150frame.gif
14-Nov-16 12
Brownian Motion
14-Nov-16 13
Reproduced from the book of Jean Baptiste Perrin, Les Atomes, three tracings of the motion of colloidal particles of radius 0.53 Β΅m, as seen under the microscope, are displayed. Successive positions every 30 seconds are joined by straight line segments (the mesh size is 3.2 Β΅m)
Brownian Motion
14-Nov-16 14
ππ9π₯ππ‘9 = βπΌ
ππ₯ππ‘ + πΉ(π‘) πΌ = 6πππ
Brownian Motion
14-Nov-16 15
ππ9π₯ππ‘9 = βπΌ
ππ₯ππ‘ + πΉ(π‘) πΌ = 6πππ
π2π9π₯9
ππ‘9 βπππ₯ππ‘
9= β
πΌ2ππ₯9
ππ‘ + π₯πΉ(π‘)
Brownian Motion
14-Nov-16 16
ππ9π₯ππ‘9 = βπΌ
ππ₯ππ‘ + πΉ(π‘) πΌ = 6πππ
π2π9π₯9
ππ‘9 βπππ₯ππ‘
9= β
πΌ2ππ₯9
ππ‘ + π₯πΉ(π‘)
Define π½ = DEF
DG
π2ππ½ππ‘ β π
ππ₯ππ‘
9= β
πΌ2 π½ + π₯πΉ(π‘)
Brownian Motion
14-Nov-16 17
ππ9π₯ππ‘9 = βπΌ
ππ₯ππ‘ + πΉ(π‘) πΌ = 6πππ
π2π9π₯9
ππ‘9 βπππ₯ππ‘
9= β
πΌ2ππ₯9
ππ‘ + π₯πΉ(π‘)
Define π½ = DEF
DG
π2ππ½ππ‘ β π
ππ₯ππ‘
9= β
πΌ2 π½ + π₯πΉ(π‘)
π2ππ½ππ‘ β πIπ = β
πΌ2 π½
Brownian Motion
14-Nov-16 18
ππ9π₯ππ‘9 = βπΌ
ππ₯ππ‘ + πΉ(π‘) πΌ = 6πππ
π2π9π₯9
ππ‘9 βπππ₯ππ‘
9= β
πΌ2ππ₯9
ππ‘ + π₯πΉ(π‘)
Define π½ = DEF
DG
π2ππ½ππ‘ β π
ππ₯ππ‘
9= β
πΌ2 π½ + π₯πΉ(π‘)
π2ππ½ππ‘ β πIπ = β
πΌ2 π½ π½ =
2πIππΌ + π΄πL
MGNβ
Brownian Motion
14-Nov-16 19
ππ9π₯ππ‘9 = βπΌ
ππ₯ππ‘ + πΉ(π‘) πΌ = 6πππ
π2π9π₯9
ππ‘9 βπππ₯ππ‘
9= β
πΌ2ππ₯9
ππ‘ + π₯πΉ(π‘)
Define π½ = DEF
DG
π2ππ½ππ‘ β π
ππ₯ππ‘
9= β
πΌ2 π½ + π₯πΉ(π‘)
π2ππ½ππ‘ β πIπ = β
πΌ2 π½ π½ =
2πIππΌ + π΄πL
MGN
π₯9 =2πIππΌ π‘ =
2πIπ6πππΌ π‘
β
Brownian Motion
14-Nov-16 20
ππ9π₯ππ‘9 = βπΌ
ππ₯ππ‘ + πΉ(π‘) πΌ = 6πππ
π2π9π₯9
ππ‘9 βπππ₯ππ‘
9= β
πΌ2ππ₯9
ππ‘ + π₯πΉ(π‘)
Define π½ = DEF
DG
π2ππ½ππ‘ β π
ππ₯ππ‘
9= β
πΌ2 π½ + π₯πΉ(π‘)
π2ππ½ππ‘ β πIπ = β
πΌ2 π½ π½ =
2πIππΌ + π΄πL
MGN
π₯9 =2πIππΌ π‘ =
2πIπ6πππΌ π‘ π9 =
4πIππΌ π‘ =
4πIπ6πππΌ π‘
β
β
Brownian Motion
14-Nov-16 24
π9 =4πIππΌ π‘ =
4πIπ6πππΌ π‘
π = 8.90Γ10LX Pa $ π π = 1.1 ππ
Brownian Motion
14-Nov-16 25
π9 =4πIππΌ π‘ =
4πIπ6πππΌ π‘ β πI =
πππ·π‘
6πππ4π ~1.1Γ10L9aπ½/πΎ
π = 8.90Γ10LX Pa $ π π = 1.1 ππ
Advanced Labs - Zeeman Effects
Zhenyu Ye
14-Nov-16 26
Experiments in Modern Physics β A. Melissinos Chapter 6
Modeling of Hydrogen Atoms
14-Nov-16 27
n Schrodinger equation in 1926
i! ββtΞ¨!r, t( ) = β!2
2mβ2 +V !r, t( )
β‘
β£β’
β€
β¦β₯β Ξ¨
!r, t( )
Ξ¨!r( ) = 1
rβ Ο l r( ) β Ylm ΞΈ,Ο( )
En = βe2
!cβ
ββ
β
β β
2mec
2
2n2
m = 0,Β±1,!,Β±l
L = l(l +1)! Lz =m!
l = 0,1,!,nβ1n =1,2,!
See Adv.Lab.2
Electron Spin
14-Nov-16 28
S = s(s+1)! s = 12
1925: G.Uhlenbeck, S.Goudsmit
Sz =ms! ms = Β±12
π½=πΏ+π
πg=πh +πi
Electron Spin
14-Nov-16 29
S = s(s+1)! s = 12
Ag Shell Structure: 2, 8, 18, 18, 1
1925: G.Uhlenbeck, S.Goudsmit
Sz =ms! ms = Β±12
Stern-Gerlach Experiment 1922
π½=πΏ+π
πg=πh +πi
Electron Spin
14-Nov-16 30
S = s(s+1)! s = 12
Ag Shell Structure: 2, 8, 18, 18, 1
1925: G.Uhlenbeck, S.Goudsmit
Sz =ms! ms = Β±12
Stern-Gerlach Experiment 1922
Bohr magneton πI =jβ9N
πm = 1
πn = 2
πh = πmπmπI
πi = πnπnπI
πΈp,Nr,Ns = βπ9
βπ
9πjπ9
2π9 + πhπ΅ + πiπ΅
L, S and J
14-Nov-16 31
2S+1LJ
541.6nm
S=1, L=0, J=1
S=1, L=1, J=2
π½=πΏ+π
πg=πh +πi
L, S and J
14-Nov-16 32
πg =πi $ π + πh $ πΏ
π + πΏ
2S+1LJπΈ = πΈIvw + πgπ΅
βπΈ = β(πgπg)πIπ΅
541.6nm
π½=πΏ+π
πg=πh +πi
πg = πgπgπI
L, S and J
14-Nov-16 33
ΞJ=Β±1, Ξmj=0, Β±1
2S+1LJ
541.6nm
π½=πΏ+π
πg=πh +πi
πg =πi $ π + πh $ πΏ
π + πΏ
πΈ = πΈIvw + πgπ΅
βπΈ = β(πgπg)πIπ΅
πg = πgπgπI
Fabry-Perot Etalon
14-Nov-16 37
ππ = 2ππππ π = 2π 1 β π ππ9π β 2π 1βπ9
2 β 2π 1βπ·~9
8π9
Wave-length Shift Calculation
14-Nov-16 38
βπ =π9
2ππ·~a9 β π·~99
π·~LοΏ½9 β π·~99=π9
2ππ·~99 β π·~οΏ½9
π·~LοΏ½9 β π·~99