↓↓ ↑
↑↓
"M"
↳ "Mmin-1"
mini
"Michaelis"
perf (Vmax of diff)
·
Sequential b(EAB = EPQ) (yp450Linetic = rate
[S] < km
Baka
↳ Stabilize the TS (not Grxn) /↑ ran speed
↳ destabilize ground state
↓
I↳ G of
1
↳entrnP
↳ microenvironment
↳ covalent bend
Iz
Vmax
-
Ka is only
associate of substrate
limited by
to
rate
enz
egsammaparebap
instead
↳ waves prod diffraction patterns (notparticle) /e
-
unti distribute v
peak
↳ single e-behave like both slits (fblock choose)
waves - > can
-
whenheae
I I
Black
Body Radiation
(intensityS
↑ Photoelectric Effect Atomic Line Specte
shine light knock offer diffelements specific color lines
-
as X-0-
hot bodies radiate
light "See Energy leve quantized
-
light intensity support
>
above depends >
KE on
4E Ef Ei hux
M
observed has peak dep on temp .# ofe is
= =
proportionalto
-
>
1
intensiti ->> absorption E; <Ef -
: us us
light is quantized(lighthasanyofE2 . KE ofedepends Frequency of light emission Ei)EfE
on :
Emol Photo
1 photon
=
EphxNa 3 No e-are
.
exected below frequency
Threshold
= Rhint =
Ephhreject
N
↓ (When
Cam
>
light balb (infared/same
"White
as Earth
e- Lymann :
Nf = 1 Balmer :
; Rf = 2
assume afte Sun)
or + Lower X- high F, EDKE *
Paschen : nf = 3; Bracket: nf = 4
Acut = Auncat
> not KE Can used for any H-like atan
Quiz 3
- a
+ Lower intensity > ↓ #photenz (Het Lit
-
>
; ,
...
Note : If
Heisenberg de Broglie *
find Spatial location "discrete"
X for ejection A
:
? = 0- .
&
↳ KE h =E
particle associated w/X =
Mev X 578
particle nature of matter
waves nature of
:
light "spread"
= am
findrefective Rule of combination
:
apphot If
·
X "NO MASS" -
↳ no e-eject
small&(p mu) Waves A A sin(x +1) * A part + 1 part 2part
large p
=
> >
- =
-
=
"Often insignificant 3x108 ms- "He wave 1 + wave I can be
↑
small p
X v/vaccum c= X /(f)=I Light electromagnetic
long "significant"
> V= :
> >
-
& .
.
as
↓
sin(x + 4) Eg sin (x +=)
like -"I
mass > ↑X
Phase Shift Y Ez
-
= =
"small mass mass ofe > 4v-x
-
:
HI Mum Destructivesisin Mosin
Constructive sin(x) + Sin(x) = Isin
:
My =
↳ 45 °*
> 45 ofreactant
↑↓
"M"
↳ "Mmin-1"
mini
"Michaelis"
perf (Vmax of diff)
·
Sequential b(EAB = EPQ) (yp450Linetic = rate
[S] < km
Baka
↳ Stabilize the TS (not Grxn) /↑ ran speed
↳ destabilize ground state
↓
I↳ G of
1
↳entrnP
↳ microenvironment
↳ covalent bend
Iz
Vmax
-
Ka is only
associate of substrate
limited by
to
rate
enz
egsammaparebap
instead
↳ waves prod diffraction patterns (notparticle) /e
-
unti distribute v
peak
↳ single e-behave like both slits (fblock choose)
waves - > can
-
whenheae
I I
Black
Body Radiation
(intensityS
↑ Photoelectric Effect Atomic Line Specte
shine light knock offer diffelements specific color lines
-
as X-0-
hot bodies radiate
light "See Energy leve quantized
-
light intensity support
>
above depends >
KE on
4E Ef Ei hux
M
observed has peak dep on temp .# ofe is
= =
proportionalto
-
>
1
intensiti ->> absorption E; <Ef -
: us us
light is quantized(lighthasanyofE2 . KE ofedepends Frequency of light emission Ei)EfE
on :
Emol Photo
1 photon
=
EphxNa 3 No e-are
.
exected below frequency
Threshold
= Rhint =
Ephhreject
N
↓ (When
Cam
>
light balb (infared/same
"White
as Earth
e- Lymann :
Nf = 1 Balmer :
; Rf = 2
assume afte Sun)
or + Lower X- high F, EDKE *
Paschen : nf = 3; Bracket: nf = 4
Acut = Auncat
> not KE Can used for any H-like atan
Quiz 3
- a
+ Lower intensity > ↓ #photenz (Het Lit
-
>
; ,
...
Note : If
Heisenberg de Broglie *
find Spatial location "discrete"
X for ejection A
:
? = 0- .
&
↳ KE h =E
particle associated w/X =
Mev X 578
particle nature of matter
waves nature of
:
light "spread"
= am
findrefective Rule of combination
:
apphot If
·
X "NO MASS" -
↳ no e-eject
small&(p mu) Waves A A sin(x +1) * A part + 1 part 2part
large p
=
> >
- =
-
=
"Often insignificant 3x108 ms- "He wave 1 + wave I can be
↑
small p
X v/vaccum c= X /(f)=I Light electromagnetic
long "significant"
> V= :
> >
-
& .
.
as
↓
sin(x + 4) Eg sin (x +=)
like -"I
mass > ↑X
Phase Shift Y Ez
-
= =
"small mass mass ofe > 4v-x
-
:
HI Mum Destructivesisin Mosin
Constructive sin(x) + Sin(x) = Isin
:
My =
↳ 45 °*
> 45 ofreactant
