, Mnr spectroscopy
B spin a
I
'
wagon::uT:ak:L
I
- mm .
it
.
These nuclei have T T
property
-
a
called absorb
spin which can
d
spin Bo
radio
frequency radiation when
appropriate magnetic field is
to it Stable and lower
applied in
^
energy
.
.
I
B spin with Bo
DE States the
aligned
' a states
spin ones
= -
the
DE
directly dependent on OE T with Bo 't
strength of the magnetic field .
how does it top spin state ?
go from a
All we need is
Radiofrequency energy .
B t
g)
If the nuclei
falls back
from the B state to
y
y yer .
the
is
a
released
state ,
some radio
frequency energy
17
.
This continues known
energy enchange
is as
peg
Nuclear Resonance
resonance and hence
Magnetic .
B spin a
I
'
wagon::uT:ak:L
I
- mm .
it
.
These nuclei have T T
property
-
a
called absorb
spin which can
d
spin Bo
radio
frequency radiation when
appropriate magnetic field is
to it Stable and lower
applied in
^
energy
.
.
I
B spin with Bo
DE States the
aligned
' a states
spin ones
= -
the
DE
directly dependent on OE T with Bo 't
strength of the magnetic field .
how does it top spin state ?
go from a
All we need is
Radiofrequency energy .
B t
g)
If the nuclei
falls back
from the B state to
y
y yer .
the
is
a
released
state ,
some radio
frequency energy
17
.
This continues known
energy enchange
is as
peg
Nuclear Resonance
resonance and hence
Magnetic .