Skip to main content

Full text of "Transparencies Unit Unit 6 - The Nucleus: Project Physics"

See other formats


'g.'<..j».' 


^.  •>.;-  •^\y" 


■"  ■■'■vs.  ^r^^S^i^ 


v; 


«sS 


PROJECT  PHYSICS 

TRANSPARENCIES  UNIT  6 

Authorized  Interim  Version 


HOLT,  RINEHART  &  WINSTON,  INC. 


1 809250 


Harvard  Project  Physics 
Overhead  Projection  Transparencies 

Unit  6 
T40       Separation  of  Q,  0,  y  rays 
T41       Rutherford's  a -Particle  "Mousetrap" 
T42       Radioactive  Disintegration  Series 
T43       Radioactive  Decay  Curve 
T44       Radioactivity  Displacement  Rules 
T45       Mass  Spectrograph 
T46       Chart  of  the  Nuclides 
T47       Nuclear  Equations 
T48       Binding  Energy  Curves 


140 


T40  Separation  of  a,  /S,  y  Rays 


T40 


Separation  of  a ,  3 ,  7  Rays 


With  this  transparency  one  may  discuss  the  effect  of  a  magnetic  field  on  the  emanations  coming  from  a 
radioactive  source.  The  obsei-ved  deflections  are  presented  without  identification  to  pennit  the  student 
to  apply  his  knowledge  of  the  behavior  of  charged  particles  in  a  magnetic  field,  (see  T32  Unit  4) . 

Overlay  T40-A  Shows  an  electromagnet  (with  cuiTent  off)  surrounding  a  lead-shielded  source  of  ra- 
dio-activity. When  no  magnetic  field  is  present  only  one  path  of  radiation  is  observed. 
Introduce  overlay  T40-B. 

Overlay  T40-B  Shows  the  effect  of  a  moderate  magnetic  field  strength  on  the  emanations.  Since  a  de- 
flection occurs,  it  must  be  true  that  this  emanation  possesses  charge.  Ask  students  to 
apply  the  right  hand  and  left  hand  rules  to  determine  the  charge  on  this  ray.  It  will 
be  seen  that  the  left  hand  rule  is  applicable  since  the  force  is  upward  and  conse- 
quently the  charge  is  negative.  It  is,  of  course,  the  $  ray. 
Note:  Beta  rays  exhibit  a  continuous  distribution  of  energies.  We  have  indicated 

betas  of  only  one  energy  here  for  simplicity. 
Remove  overlay  T40-B  and  introduce  overlay  T40-C. 

Overlay  T40-C  Shows  the  effect  of  a  more  intense  magnetic  field  on  the  radioactive  emanations.  A  new 
deflection  is  noted  which  necessarily  is  positive  since  it  is  opposite  to  the  deflections 
of  the  B  rays.  The  degree  of  deflection  shows  that  this  positive  ray,  the  G  ray,  has  a 
much  larger  momentum  than  tha  t  of  the  /S's.  Point  out  that  the  decrease  in  the  radius 
of  the  $'s  is  a  result  of  the  increa  sed  B  field.  Additionally,  have  students  comment  on 
the  undeflected  ray.  Indicate  that  further  increases  in  the  magnetic  field  strength 
will  not  affect  this  ray,  although  the  other  two  would  continue  to  be  affected.  This  un- 
deflected ray  is,  of  course,  the  neutral  y  ray. 


T-40 


T-40— 

/ 


Tt4So 


T41 


T41  Rutherford's  0 -Particle  "Mousetrap" 


T41  Rutherford's  a-Particle  "Mousetrap" 

This  transparency  presents  a  simplified  detail  of  the  apparatus  used  by  Rutherford  and  Royds  in  1909 
to  show  that  the  Q  particle  is  a  doubly-ionized  helium  atom,  that  is,  the  nucleus  of  a  He  atom. 

Overlay  T41-A  Shows  a  thick-walled  glass  chamber  leading  to  a  discharge  tube  at  the  top.  In  the 
lower  portion  is  a  thin-walled  tube  one  hundreth  of  a  millimeter  thick  containing  ra- 
don gas.  The  outer  tube  was  evacuated  and  the  apparatus  was  allowed  to  stand  for  a 
week.  As  time  passed,  Cf  particles  from  the  radon  gas  traveled  through  the  thin- 
walled  tube  into  the  evacuated  chamber.  Here  the  "  CI  particle  gas"  was  compressed 
into  the  discharge  tube  by  means  of  a  mercury  column  not  shown.  A  potential  dif- 
ference was  maintained  across  the  electrodes  and  an  electric  discharge  was  produced 
in  the  "gas".  The  resulting  light  was  examined  with  a  spectroscope.  Introduce  over- 
lay T41-B  with  a  mask. 

Overlay  T41-B  Illustrates  more  Q  particles  in  the  discharge  tube  and  suggests  light  emanating  from 
the  tube.  The  right  side  of  the  overlay  provides  the  spectra  which  wei'e  observed 
as  time  went  on.  Reveal  each  spectrum  separately  by  sliding  an  opaque  mask  down 
the  overlay.  The  final  spectrum  is  a  comparison  spectrum  of  helium.  Discuss  the  in- 
tei-pretation  of  these  results. 

Note:  You  may  wish  to  add  the  actual  colors  to  the  spectral  lines.  This  can  be  done 
with  colored  wax  pencils,  felt  markers,  or  colored  tapes.  Refer  to  T39  Unit  4 
for  exact  coloration. 


1^-T 


IM  lAT 


T42  Radioactive  Disintegration  Series 
T42 


V 


T42 


Radioactive  Disintegration  Series 


This  transparency  will  be  useful  in  discussing  the  process  of  radioactive  transmutation  which  elements 
undergo  by  emitting  G  and  $  particles.  Four  series  are  presented :  Uranium-Radium ;  Thorium ;  Actin- 
ium; Neptunium.  It  is  intended  that  this  transparency  be  completed  by  the  teacher  (with  a  wax  pen- 
cil) as  students  consult  the  Periodic  Table  and  determine  the  complete  symbol  with  A  and  Z  for  each 
member  of  the  series. 

Overlay  T42-A  Shows  the  principal  components  in  the  Uranium  Series.  U-238  emits  an  0  particle  re- 
sulting in  an  element  possessing  90  protons  and  234  nucleons.  Element  90  is  Tho- 
rium. Therefore,  the  symbol  yoTh^'^  is  placed  in  the  first  blank  circle.  Th-234  then 
emits  a  $  particle  resulting  in  an  element  with  91  protons  and  234  nucleons.  Accord- 
ing to  the  Periodic  Table  element  91  is  Protactinium;  therefore,  ,„Pa-''  is  placed  in 
the  second  circle.  The  procedure  continues  in  a  similar  manner  until  the  stable  daugh- 
ter is  reached. 

In  this  series  some  points  are  reached  by  a  process  called  "branching";  a  small 
fi-action  of  atoms  decay  in  a  manner  other  than  that  shown.  The  branching  in  this 
series  is  as  follows: 


Th 


.34  — B   ,    p^234  — B_^  u" 


Bi2w  — g_^  rppio  — §_ 


Pb-"'  *^—  Bi^ 


Remove  overlay  T42-A  and  introduce  overlay  T42-B. 

Overlay  T42-B      Shows  the  scheme  for  the  Thorium  Series.  Follow  the  same  procedure  as  in  overlay 
T42-A.  The  bi'anching  in  this  series  is  as  follows: 


B 


AV-' 


Po-'"  - 

Bi2.2  B        ,       Po-M 


a 


^  Bi^ 


-^  Pb™« 


Remove  overlay  T42-B  and  introduce  overlay  T42-C. 

Overlay  T42-C      Shows  the  scheme  for  the  Actinium  Series,  so-called  because  U-235  was  once  known 
as   Actinouranium.   The   branching  in  this  series  is  as  follows: 


Ac^ 
Po^ 


B 


Th^ 


-*  At^ 


a 


-i^  Ra=^ 


115       Q   ^   Bi^^^  ■ 


Po^ 


a 


-i-Pb^ 


Remove  overlay  T42-C  and  introduce  overlay  T42-D. 
Overlay  T42-D      Shows  the  scheme  for  the  Neptunium  series.  The  branching  is  as  follows: 


Bi"^ Q    ,    Tl^"-' ^-^  Pb^ 


T-42 


92 


cc 


238 


\ 


Uranium  Series 


ct 


/ 


/ 


<^^^~^ 


^\      )^(      )^\      )^. 


stable 


T-42 


A 


T-42 


T-42 


Neptunium  Series 


CL 


CL 


241 


y 


PuU 


'      - ,      ^ 


\ 


^\jO 


( 


y 


stable 


T43  Radioactive  Decay  Curve 


T43 


T43 


Radioactive  Decay  Curve 


Use  this  transparency  to  aid  in  the  discussion  of  the  half-life  concept  in  radioactive  decay.  A  number 
of  overlays  displaying  sample  data  for  a  radioactive  element  and  its  accumulating  "daughter"  atoms 
are  presented  for  analysis. 


Overlay  T43-A 


Overlay  T43-B 


Overlay  T43-C 


Overlay  T43-D 

to 
Overlay  T43-F 


Shows  the  axes  on  which  data  for  surviving  and  accumulating  atoms  will  be  plotted. 
The  vertical  axis  represents  numbers  of  atoms,  No  being  the  original  quantity.  The 
horizontal  axis  is  in  arbitrary  time  units.  Introduce  overlay  T43-B. 

Shows  plotted  data  for  the  surviving  parent  atoms  and  the  accumulating  daughter 
atoms  for  a  short  time  interval.  Point  out  that  as  radioactive  decay  occurs,  the  orig- 
inal radioactive  atoms  transmute  into  new,  in  this  case  stable,  atoms.  The  plot 
shows  this  increasing  number  of  daughter  atoms  along  with  the  remaining  num- 
ber of  parent  atoms.  Add  overlay  T43-C. 

As  time  goes  on,  more  parent  atoms  decay  into  new  daughter  atoms.  This  overlay 
shows  that  the  number  of  daughter  atoms  eventually  becomes  equal  to  the  number  of 
remaining  parent  atoms.  Add  overlay  T43-D. 

As  time  progresses,  the  number  of  daughter  atoms  is  seen  to  increase  further  while 
the  number  of  surviving  parent  atoms  is  shown  decreasing.  Continue  with  the  re- 
mainder of  the   overlays. 

Now  that  you  have  presented  the  complete  data  for  the  graph  you  can  indicate 
the  suggestion  of  Rutherford  that  it  is  possible  to  specify  the  time  required  for  any 
particular  fraction  of  a  radioactive  substance  to  decay  to  one-half,  one-third,  or  one- 
fourth  of  the  original  quantity.  The  fraction  1/2  has  been  chosen  for  convenience 
and  the  time  T  thus  required  is  called  the  half-life.  It  is  the  time  during  which  a  ra- 
dioactive material  decays  to  one- half  of  its  original  amount. 

Ask  students  to  point  out  the  half-life  from  the  graph.  It  is  20  time  units.  Remove  over- 
lays T43-F-E-D  and  show  that  the  number  of  atoms  I'emaining  after  20  time  units  have 
elapsed  is  No/2.  Return  T43-D  and  show  that  at  the  end  of  another  20  units  of  time 
(one  half -life)  the  number  of  atoms  remaining  is  y.^  the  original  [V2(No/2)  =  y^ 
No] .  Return  overlay  T43-E  and  show  that  after  another  half-life  (20  time  units)  the 
number  of  atoms  is  V2  the  original  [1^  (14  No)  =  i/g  No].  Finally  show  that  overlay 
T43-F  illustrates  another  half -life  [l/2*'(i/8No)  =  1/16  No]. 


T-43 


Time 


Number  of  Surviving 
Parent  Atoms 


Number  of  Accumulating 
Stable  Daughter  Atoms 


T-43 


Time 


Number  of  Surviving 
Parent  Atoms 


//Number  of  Accumulating 
Stable  Daughter  Atoms 


T43 


A 

B 
C 


Time 


T4I 


Number  of  Surviving 
Parent  Atoms 


/^Number  of  Accumulating 
Stable  Daughter  Atoms 


f« 


Time 


Number  of  Surviving 
Parent  Atoms 


0 
/'^^Number  of  Accumulating 

Stable  Daughter  Atoms 


\^ 


A 

6 

C 

ID 
E 


Time 


Number  of  Surviving 
Parent  Atoms 


9 

/^Number  of  Accumulating 
Stable  Daughter  Atoms 


Time 


Number  of  Surviving 
Parent  Atoms 


/^Number  of  Accumulating 
Stable  Daughter  Atoms 


1F4I1 


Time 


Number  of  Surviving 
Parent  Atoms 


T^ 


A 

B 
C 
D 
E 


Time 


Number  of  Surviving 
Parent  Atoms 


Number  of  Accumulating 
Stable  Daughter  Atoms 


T4S 


Time 


T44  Radioactive  Displacement  Rules 


T44 


T44 


Radioactive  Displacement  Rules 


This  transparency  will  be  useful  in  leading  a  teacher-directed  discussion  of  the  Displacement  Rules  of 
Radioactivity.  Space  is  provided  to  write  in  more  examples  of  each  type  of  decay:  alpha  decay,  beta- 
decay,  and  beta+  decay. 

Overlay  T44-A  Shows  the  first  rule  in  a  visualized  "before-after"  diagram.  Before  the  a  particle  is 
ejected,  the  radioactive  nucleus  contains  A  nucleons,  Z  of  which  are  protons.  After 
the  a  is  emitted,  the  nucleus  possesses  4  less  nucleons,  2  of  which  are  protons.  The 
nucleus  is  now  a  new  element  of  atomic  number  Z-2.  Introduce  T44-B  with  a  mask. 

Overlay  T44-B  Shows  the  Cf  decay  displacement  rule  in  the  fonn  of  a  general  equation.  Below  is  a 
specific  example.  Mask  the  Th-234  and  ask  students  to  present  the  result.  Space  is 
provided  for  writing-in  further  examples: 

ggRa"-' ►seRn^^"   +  ,He' 

8331^1^ ^8,T12««     +  ,He^ 

Remove  overlays  T44-A  and  B.  Introduce  overlay  T44-C. 

Overlay  T44-C  Shows  the  second  rule  in  a  visualized  "before-after"diagram.  Before  the  $~  particle  is 
ejected,  the  radioactive  nucleus  contains  A  nucleons,  Z  of  which  are  protons.  After  the 
B~  is  emitted,  the  nucleus  retains  its  original  mass  number  but  increases  its  atomic 
number  by  one  unit.  An  antineutrino  V  is  also  given  off  but  it  does  not  affect  A  to  Z. 
Introduce  T44-D  with  a  mask. 

Overlay  T44-D  Shows  the  B~  decay  displacement  rule  in  the  form  of  a  general  equation.  Below  is  a 
specific  example.  Mask  the  Pa-234  and  ask  students  to  present  the  result.  Space  is 
provided  for  writing  in  further  examples: 


sBi"^- 
.Pu"' 


-^84Po"^    +    _ie»    +   V 


■^  95Am-"  +  -ie°   -f  V 


Remove  overlays  T44-C  and  D.  Introduce  overlay  T44-E. 

Overlay  T44-E  Shows  the  third  rule  in  a  visualized  "before-after"  diagram.  Before  the  positron  is 
ejected,  the  radioactive  nucleus  contains  A  nucleons,  Z  of  which  are  protons.  After  the 
j5+  is  emitted,  the  nucleus  retains  its  original  mass  number  but  decreases  its  atomic 
number  by  one  unit.  A  neutrino  V  is  also  given  off  but  it  does  not  affect  A  or  Z.  In- 
troduce T44-F  with  a  mask. 

Overlay  T44-F  Shows  the  /S"'"  decay  displacement  rule  in  the  fonn  of  a  general  equation.  Below  is  a 
specific  example.  Mask  the  Si-30  and  ask  students  to  present  the  result.  Space  is  pro- 
vided for  writing-in   further  examples: 


rN' 


—  eC"     -f     ^eo     -f    V 


9F" -«0i«     _|-     ,e°     -f    V 


T-44 


BEFORE 


CL 


DECAY 


AFTER 


T44 


BEFORE 


CL 


DECAY 


AFTER 


92 


u 


238 


» 


Jh'''+He 


T-44 


BEFORE 


ft 


DECAY 


AFTER 


T^44 


DECAY 


AFTER 


Y'+,e°+i) 


Jh 


234 


*.,PaV,e°+i) 


T-44 


DECAY 


TF44W 


BEFORE 


ft- 


DECAY 


AFTER 


15 


P 


30 


S*^*^  I  0  I 


T45  Mass  Spectrograph 


T45 


T45 


Mass  Spectrograph 


A  schematic  diagram  of  the  apparatus  known  as  the  mass  spectrograph  is  presented  in  this  transpar- 
ency. Overlays  ilkistrate  the  operation  of  the  velocity  selector  and  the  mass-determining  section  of  the 
spectrograph. 


Overlay  T45-A 


Overlay  T45-B 


Shows  the  arrangement  of  magnetic  and  electric  fields  used  to  select  ions  of  a  certain 
Sliced.  The  electric  and  magnetic  forces  on  ions  in  the  beam  are  in  opposite  direc- 
tions. The  magnitude  of  the  magnetic  force  increases  with  the  speed  of  the  ions.  Only 
those  ions  on  which  the  magnitude  of  the  magnetic  force  equals  the  magnitude  of  the 
electric  force  will  be  undeflected  and  pass  through  the  slit.  Three  beams  are  shown, 
one  of  ions  moving  too  slowly,  one  of  ions  moving  too  rapidly,  and  one  of  ions  moving 
at  just  the  right  speed  to  pass  through  the  slit.  For  these  ions  F  mag  =  F  elect,  that 
is,  qvB  -  qE.  So  the  speed  of  ions  going  through  the  sUt  is  v  =  E/B.  Introduce  overlay 
T45-B. 

Shows  an  undeflected  beam  passing  through  the  slits  and  entering  a  second  magnetic 
field  B' produced  by  a  separate  magnet.  The  beam  is  now  acted  on  only  by  this  mag- 
netic field  which  will  cause  it  to  follow  a  circular  path.  The  centripetal  force  is  sup- 
plied by  the  magnetic  force  qvB'  =  mv-/R-  The  mass  can  now  be  determined  by  solv- 
ing for  m  and  substituting  v  =  E/B  into  the  equation.  Thus 

m   =     qBB'R 
E 


The  radius  of  curvature  R  can  be  measured  with  the  aid  of  the  film  pack.  The  values 
B,  B'  and  E  are  determined  from  the  design  of  the  apparatus,  and  measurements  of 
magnet  current  and  plate  voltage. 


T-45 


T45 


T46 


T46  Chart  of  the  Nuclides 


T46 


Chart  of  the  Nuclides 


This  transparency  is  based  upon  the  "Chart  of  the  Nuchdes"  pubHshed  by  the  Knolls  Atomic  Power  Lab- 
oratory, Schenectady,  New  York.  It  represents  a  plot  of  stable  and  unstable  radioisotopes  with  other 
pertinent  nuclear  information. 

Overlay  T46-A  Shows  a  g-rid  with  a  vertical  axis  indicating  the  number  of  protons  or  the  atomic 
number  and  the  horizontal  axis  giving  the  number  of  neutrons  or  A-Z.  Add  overlay 
T46-B. 

Overlay  T46-B       Shows  the  positions  of  the  265  stable  nuclides.  Add  overlay  T46-C. 

Overlay  T46-C  Shows  the  positions  of  those  radioactive  nuclides  which  occur  naturally.  Add  over- 
lay T46-D. 

Overlay  T46-D  Shows  the  positions  of  the  265  stable  and  approximately  1130  radioactive  isotopes. 
Add  overlay  T46-E. 

Overlay  T46-E  Shows  a  line  plotting  nuclides  which  contain  equal  numbers  of  protons  and  neutrons. 
Those  nuclides  with  small  atomic  numbers  lie  on  this  line  while  those  of  higher 
atomic  number  possess  more  neutrons  than  protons.  Add  overlay  T46-F. 

Overlay  T46-F  Shows  those  nuclides  with  nuclei  possessing  2,  8,  20,  50,  or  82  protons,  or  2,  8,  20,  50, 
82  or  126  neutrons.  These  nuclides  are  unusually  stable.  The  numbers  are  referred  to 
as  "magic  numbers".  Remove  overlays  T46-F-E-D-C  and  introduce  overlay  T46-G. 


Overlay  T46-G      Shows  a  simplified  detail  of  the  chart  indicating  stable  nuchdes  (large  numbers)  and 
those  radioactive  nuclides  which  experience  positron  decay  and  k -capture. 


J-A6 


NUMBER  OF  NEUTRONS  (A-Z) 


-rT4fB 


A 
B 


NUMBER  OF  NEUTRONS  (A-Z) 


-MB 


NUMBER  OF  NEUTRONS  (A-Z) 


nw 


<   40 


Stable  and  Radioactive 
Nuclides 

^           "  f 

k* 

mm*ma 

^' 

r 

Stable  Nu:lides 

■ 

'^' 

J- 

1  ■ 

Natural  Radioactive 
Nuclides 

^ 

■^^' 

m 

/ 

V 

NUMBER  OF  NEUTRONS  (A-Z) 


^^^^ 


120 
100 

^^^ 

32 

31 

Ge 

1 

66 

(^a 

e+ 

e+ 

«7l 

oa 

64 

65 

.jjr 

30 

Zn 

60 

61 

kfi+ 
62 

k/s^ 
63 

64 

r^ii 

/s+ 

e+ 

/S+ 

/s+k 

e+ 

^5. 

!^  so 

— ^^ 
28 

i^U 

58 

5$ 

60 

61 

62 

DD 

■■■  ■ 

Stable  Nuclides 

LU 

Ni 

k 

56 

57 

58 

k 

59 

60 

61 

■ 

■ 
■   ■    ■ 

^ 

.  jrr- 

H   H  ■  M 

z  60 

o 

I 

r 

■ 

■    ■    H 
■    ■    HM 

* 

J- 

■   ■ 

<  40 

M 

r 

20 
0 

/ 

r^- 

NUMBER  OF  NEUTRONS  (A-Z) 


T47 


T47   Nuclear  Equations 


T47 


Nuclear  Equations 


This  transparency  will  be  useful  in  presenting  the  nuclear  equations  associated  with  certain  major 
events  in  the  history  of  nuclear  physics:  the  first  artificial  transmutation;  the  discovery  of  the  neu- 
tron; and  the  mass-energy  relation. 


Overlay  T47-A 


Overlay  T47-B 


Overlay  T47-C 


Overlay  T47-D 


Shows  visualizations  for  two  nuclear  reactions:  the  upper  one  represents  the  first 
artificial  transmutation  of  an  atom  of  one  chemical  element  into  an  atom  of  another 
chemical  element;  the  lower  one  represents  the  nuclear  reaction  for  the  discovery 
of  the  neutron.  Mask  that  segment  which  is  not  being  discussed  at  the  moment.  This 
overlay  is  essentially  for  visualizing  the  capture  of  the  Q  particle  by  the  target  nu- 
cleus and  its  subsequent  transmutation  and  release  of  one  of  its  nucleons.  It  will  also 
serve  to  emphasize  the  conservation  of  charge  and  mass  number.  Introduce  overlay 
T47-B. 

Shows  the  nuclear  equations  for  these  reactions  along  with  black  spheres  to  distin- 
guish protons  from  neutrons  in  the  nucleus.  The  "compound  intermediate"  9F'*  is  in- 
cluded to  emphasize  the  capture  of  the  fl  particle  by  the  N-14  nucleus.  Remove  over- 
lays T47-A  and  B.  Introduce  overlay  T47-C. 

Shows  the  nucleons  involved  in  a  nuclear  reaction  exhibiting  a  loss  of  rest  mass.  Add 
overlay  T47-D. 

Shows  the  nuclear  equation  for  the  reaction  and  indicates  which  nucleons  are  pro- 
tons. In  addition,  the  rest  mass  of  each  nucleus  is  presented  in  ATOMIC  MASS  UNITS. 
Space  is  provided  to  compute  the  mass  defect  from  which  the  mass-energy  relation 
may  be  discussed. 


T-47 


T-47 


12 


T-47 


I- 


T-47      T-47 


H'  +  ir-CBe)-He+,He 


1.007825    7.016005 


4.002603     4.002603 


T48  Binding  Energy  Curves 
T48 


T48 


Binding-  Energy  Curves 


This  transparency  presents  plots  for  the  total  binding  energy  of  nuclei  and  the  average  binding  energy 
per  nucleon. 

Overlay  T48-A  Shows  a  grid  with  the  number  of  nucleons  in  the  nucleus  plotted  along  the  horizon- 
tal axis.  The  vei'tical  axis  will  be  determined  by  the  subsequent  overlays.  Introduce 
overlay  T48-B. 

Overlay  T48-B  Shows  a  plot  of  the  total  binding  energy  for  47  nuclides.  The  total  binding  energy  is  de- 
fined as  the  difference  between  the  sum  of  the  rest  masses  of  the  protons  and  neutrons 
in  the  free  state  and  the  rest  mass  of  the  nucleus  containing  the  same  number  of  nu- 
cleons. The  values  run  from  2.2  MeV  for  H-2  to  1803  MeV  for  U-238.  The  value  for 
Sn-120  is  1020  MeV;  for  He-4  it  is  28.3  MeV.  Remove  this  overlay  and  introduce 
T48-C. 

Overlay  T48-C  Shows  a  plot  of  the  average  binding  energy  per  nucleon  for  the  same  47  nuclides.  To 
compute  the  binding  energy  per  nucleon  simply  divide  the  previously  determined  total 
binding  energy  by  the  number  of  particles  in  the  nucleus.  The  binding  energy  per  nu- 
cleon is  seen  to  be  highest  for  the  middle  elements  —  the  most  stable  nuclei.  The 
average  binding  energy  per  nucleon  curve  is  useful  in  predicting  energy  releases  in 
nuclear  reactions.  When  the  products  of  a  nuclear  reaction  lie  higher  on  the  binding 
energy  curve  than  do  the  reactants,  they  have  more  binding  energy  per  particle  and 
release  energy  equal  to  the  increase  in  the  total  binding  energy. 





)  120  160  200 

NUMBER  OF  NUCLEONS  IN  NUCLEUS  (A) 


Total 
Binding 
Energy 

in 
MeV 


isoa 
i6oa 
i4oa 
ooa 
looa 
8oa 
6oa 

4C« 

300 

u- 

• 

• 

• 
• 

• 

• 

• 

• 

Sn'^° 

• 

• 

• 

• 

. .    4 

• 

• 
• 
• 

1 

He.. 

• 

• 

^^Q^H^E 

0               so               no              160             200             240 
NUMBER  OF  NUCLEONS  IN  NUCLEUS  (A) 

Binding 
Energy 

Per 

Nucleon 

in 

MeV 


10 

f 


i 

I 
I 


\i                /I 

c 

f 

• 

•         • 

•  • 

• 

% 

••• 

• 

^,234 

He.. 

•• 

• 

• 

• 

y2:J8 

•Li^ 

.He^ 

.H^ 

,h' 

y  120  160  200 

NUMBER  OF  NUCLEONS  IN  NUCLEUS  (A)