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He-Ne 7 _T $ [õ u § M Ç U ذ Ë ÑÌ ¦ R® Žz º › ͓ Ó Þ” X ¢ Ä Z ذ Ë Ñ à Ã Å Ä Z ØV Ä U ê s0 n É8 ý 4 ® o

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(1)

 10 Z 4, pp. 1079∼1084

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Development of a Spectrogram Analysis Method Using a He-Ne Laser as a Standard Source

Bukyung Jhun

Gyeonggi Science High School, Gyeonggi 400-210

Youngseok Jhun

Seoul National Univ. of Edu., Seoul 137-070

(Received 16 June, 2010 : revised 28 September, 2010 : accepted 15 October, 2010)

In this study, we developed a new method to analyze a spectrum quantitatively. In this way a beam of laser is used to be diffracted by the grating in the spectrometer with the light to be analyzed, so that the spot of the diffracted beam can be used as a reference for the wavelength measurement.

We first took a photo of the spectrum and then acquired a graph of intensity vs. wavelength by a computer program. Each test using sodium, argon, and hydrogen discharge tube showed a very precise result within the measurement uncertainty of 3 %. Especially, the new method does not have to use another light source as a reference, so it does not need multiple spectrum pictures. This is expected to be used in various experiments about fundamental conception of light and colour or interaction between light and matter.

PACS numbers: 01.50.Pa

Keywords: Spectrometer, Diffraction grating, Line spectrum, Spectroscopy

E-mail: [email protected]

-1079-

(2)

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(3)

Fig. 1. The range of visible spectrum lines; laser spot can be used as a reference.

s: slit - light comes through the slit.

dr: the boundary of 1st order diffracted red light.

ir: the image of 1st order diffracted red light.

dl: the boundary of 1st order diffracted laser beam.

il: the image of 1st order diffracted laser light.

dv: the boundary of 1st order diffracted violet light.

iv: the image of 1st order diffracted violet light.

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  6 £ §, % 3 # Qt   H Û ¼& 7 ˜à Ô! 3 `  ¦, slit s  † < Êa   𠏕 ¸2 Ÿ ¤  

”

 Ü ¼– Ð n ” Ü ¼€   K { © œ Û ¼& 7 ˜à Ô! 3  0 A\  Y Us $ \  _ ô  Ç  r] X  Á

º] (  _  & h Ü ¼– Ð Ò q tl l  M :ë  H \  s  כ `  ¦ l ï  r Ü ¼– Ð

# Œ q Y Vd ” `  ¦ [ jÄ º€   Û ¼& 7 ˜à Ô! 3  0 A_  y Œ • & h \  K { © œ   H y n

C_   © œ`  ¦ ½ ¨½ + É Ã º e ”  . Y Us $ \ " f ~ ½ ÓØ  ¦ ÷ &  H y n C`  ¦ f ”  ] X

 _ þ ta Å @`  ¦ : Ÿ x K  { 9  r ~  ´ à º• ¸ e ” t ë ß – s   â Ä º, › ' a ¹ 1 Ï 

\

>  u " î & h “   0 A+ « >`  ¦ ×  ¦ à º• ¸ e ” l  M :ë  H \  F g$ 3 Ä »\  ¦   6

 

x # Œ y n C_  [ jl \  ¦ ± ú Æ ғ ¦  % i  . ‚ à Г ¦– Ð ‘ : r ƒ  ½ ¨_ 

œ

íl  é ß –> \ " f ì ø ͕ ¸^ ‰ Y Us $ \  ¦  6   x ½ + É  כ `  ¦ “ ¦ 9 % i  Ü

¼  z  ´+ « > õ & ñ \ " f ì ø ͕ ¸^ ‰ Y Us $ \ " f ~ ½ ÓØ  ¦ ÷ &  H y n C_ 

 © œs  ] j¾ ¡ § \     › ¸F Km ”  ² ú ˜ 4 R" f z  ´+ « >\   6   x ô  Ç ì ø Í

•

¸^ ‰ Y Us $ _   © œ`  ¦  – Ð  © œ`  ¦ 8 £ ¤& ñ K   ô  Ç   H & h 

`

 ¦ µ 1 Ï|  % i l  M :ë  H \   © œs  632.8 nm– Ð { 9 & ñ ô  Ç He-Ne laser\  ¦ l ï  r F g " é ¶ Ü ¼– Ð  6   x >  ÷ &% 3  .

Figure 1“ É r  r] X     A á ¤ \ " f ‘ : r, r  F g‚   Û ¼& 7 ˜à Ô! 3  _

 # 3 0 A\  ¦    · p  כ s  . ì  rF g l   © œ _  U  ´s  1200 mm s “ ¦ 1000 lines/mm_   r] X    \  ¦  6   x ô  Ç €   @ /| Ä Ì 520 mm ð 1200 mm # 3 0 A\ " f Û ¼& 7 ˜à Ô! 3 s    ± ú ˜  כ s 

“

¦, d ”  (1)\      r] X  ) a Y Us $  F g‚  “ É r spot + þ AI – Ð 980 mm t & h \  ˜ Ð{ 9   כ s  .

III. ÷ m Ç] M ö כ r Ç4 

1. ÷ m Ç] M ö X ê sV 

Figure 1“ É r ‘ : r ƒ  ½ ¨õ & ñ \ " f ] j Œ •ô  Ç ì  rF g l _  l ‘ : r ½ ¨

›

¸\  ¦    · p Õ ªa Ë >Ü ¼– Ð He-Ne laser\  ¦ l ï  r F g " é ¶ Ü ¼– Ð  6   x

% i  . ì  rF g l – Ѝ  H l ‘ : r& h Ü ¼– Ð 250 mm×250 mm×1200 mm ß ¼l _  Ì º, á s  ² ú ˜ 9e ”   H & ñ  y Œ •+ þ A l Ñ ü æ — ¸€ ª œ_   ß ¼ w n

=  © œ \  ¦  6   x % i   H X <, & ñ  y Œ •+ þ A — ¸€ ª œ_  ¿ º x 9 €  \  y Œ • y

Œ

• _ þ ta Å @õ   r] X    \  ¦ [ O u  % i  . _ þ ta Å @“ É r  ß ¼w n =  © œ  _

 # 4 \  10 mm×50 mm ß ¼l _  : £ §`  ¦ €  $  ? /“ ¦ Õ ª 0 A\ 

&

' º ú ˜± ú ˜ 2 © œ`  ¦, ± ú ˜s   ŠҘ Ð>  # Œ · ¡ ­ # Œ" f ] j Œ • % i   H X

<, _ þ ta Å @ : £ § _  ç ß –  “ É r 0.2 mm ð 0.3 mm & ñ • ¸ ÷ &• ¸2 Ÿ ¤

(4)

Fig. 2. Structure of the spectrometer with He-Ne laser as a reference light source.

›

¸] X  % i  .  r] X      H { 9 ‘ : r _  õ † < Ɠ §½ ¨ © œ“   KENIS  _

 replica+ þ A ] j¾ ¡ § Ü ¼– Ð 1000 line/mm ½ ©  `  ¦ ‚  × þ ˜ % i  .

ì

 rF g l _  ì  r K 0 p x`  ¦ Z  } s l  0 AK " f  H Ä º‚   mm{ © œ line _  à º  8  H  r] X    \  ¦  6   x K   ô  Ç . mm{ © œ line _  à º 7 £ x  €    r] X ÷ &  H y Œ •s   8 Z O # Qt l  M :ë  H s 



. ì  rF g l _  ì  r K 0 p x`  ¦ Z  } s   H ¢ ¸ ô  Ç t _  ~ ½ ÓZ O “ É r ; Ÿ ¤ s

  8 a % v“ É r Slit`  ¦  6   x   H  כ s  . ì  rF g l \  _ ô  Ç  r] X  Á

º] (  H F g " é ¶ _  % i ½ + É`  ¦   H slit _   © œs    5 gt   H + þ AI – Ð



    H X <, slit_  ; Ÿ ¤ s  V , Ü ¼€     5 gt   H % ò % i s  V , l  M : ë

 H \  ‚  " î ô  Ç Û ¼& 7 ˜à Ô! 3 `  ¦ % 3 `  ¦ à º \ O  . \ V\  ¦ [ þ t # Q l ^ ‰

~

½ ӄ  › ' a`  ¦ F g " é ¶ Ü ¼– Ð  6   x % i `  ¦ M : ë ß –[ þ t # Qt   H ‚  Û ¼& 7 ˜à Ô

! 3

“ É r slit õ  ° ú  “ É r — ¸€ ª œ`  ¦ {   H X <, ; Ÿ ¤ s  V , “ É r slit`  ¦  6   x 

€

  Û ¼& 7 ˜à Ô! 3 ‚  • ¸ ; Ÿ ¤ s  Ï ã T“ É r } Œ •@ / — ¸€ ª œ`  ¦ s Ò  ¦  כ s  . ô  Ç

¼

# , slit_  ; Ÿ ¤ s  a % v Ü ¼€    8 ± ú ˜ – Ðî  r ‚  Û ¼& 7 ˜à Ô! 3 `  ¦ % 3 `  ¦ Ã

º e ”    H  © œ& h s  e ” t ë ß – & h “ É r € ª œ_  y n Cs  { 9   l  M : ë

 H \   © œ@ /& h Ü ¼– Ð µ 1 ßl  €  •ô  Ç Û ¼& 7 ˜à Ô! 3 ‚  “ É r › ' a ¹ 1 Ï l 

#

Q 90 >”   . s  ë  H ] j  H ì  rF g l _  U  ´s \  ¦ Z þ t # Œ" f K   ½ + É Ã

º e ”  . ì  rF g l _  U  ´s  Z þ t # Q €    r] X     A á ¤ \ " f ˜ Ð



 H slit _  r y Œ •(go)s   Œ • t l  M :ë  H \  slit_  ; Ÿ ¤ s  › ¸F K V ,

# Qt  8 • ¸ ± ú ˜ – Ðî  r ‚  Û ¼& 7 ˜à Ô! 3 `  ¦ % 3 `  ¦ à º e ”  . ‘ : r

ƒ

 ½ ¨\ " f  H µ 1 ߓ ¦ ± ú ˜ – Ðî  r  © œ`  ¦ % 3 l  0 AK " f ì  rF g l _  U

 ´s \  ¦ Ø  æì  r y  U  ´>  # Œ ] j Œ • % i  . œ íl  z  ´+ « >`  ¦   H

•

¸×  æ ì  rF g l _  ? /Â Ò # 4 \  ì ø Í   ) a y n Cs  › ' a8 £ ¤ ÷ &# Q s \  ¦ ~ ½ Ó t

 l  0 AK  Mask\  ¦ [ O u  % i  . Mask  H € 9 כ ¹\     z 

´+ « >`  ¦ €  " f Æ ÒK   ç ß –  כ s Ù ¼– Ð Fig. 2\ " f Å Ò# Q

”

  Mask_  0 Au   H þ j& h › ¸| s   u  ´ à º e ”  .

2. Ä Z ØV Ä U ê s0 n É

Û

¼& 7 ˜à Ô! 3 _   © œ\    É r y © œ• ¸\  ¦ ì  r$ 3  l  0 AK " f ' Ÿ § > =

`

 ¦  À ҍ  H X < & h ½ + Ëô  Ç á Ôo J ?# Q“   GNU Octave_  image package \ " f imread l 0 p x`  ¦ s 6   x % i  . imread l 0 p x“ É r jpg s p t  { 9 _  y Œ • i ” ! s q_  À 1 Ïy © œ, œ í2 Ÿ ¤, | ½ ÓÒ  o_  [ jl 

\

 ¦ 0∼255 _  Õ ü w  – Ð ¨ 8 Š í ß – # Œ n × m × 3_  ' Ÿ § > =– Ð   ? /



 H l 0 p x s  . n t _ O  B j – Ð n ” “ É r  ”  `  ¦ imread l 0 p x

Fig. 3. A sample picture of spectrum of which the method is induced.

Fig. 4. Sample graph of spectrum and reference beam.

Diffracted laser peak is placed at 632.8 nm.

Ü

¼– Ð ' Ÿ § > =– Ð Ô  ¦  Qü < sum " î § î # Q\  ¦  6   x K  \ P \    É r y n C _

 [ jl (À 1 Ïy © œ, œ í2 Ÿ ¤, | ½ ÓÒ  o_  [ jl _  ½ + Ë)\  ¦ ½ ¨ô  Ç Ê ê Õ ª A

á Ô\  ¦ Õ ª§ 4  .

IV. ÷ m Ç] M ö+ s ÇÊ Ý

Figure 3“ É r ‘ : r ƒ  ½ ¨\ " f > hµ 1 Ïô  Ç ì  rF g  © œu \  ¦ s 6   x 

#

Œ ë ß –[ þ t # Q”   Û ¼& 7 ˜à Ô! 3 `  ¦ O É Œ% ò ô  Ç  ”  `  ¦    · p  כ s  .

ì

 r$ 3 @ / © œ F g " é ¶“ É r + þ AF g1 p x“  X <, 0 AA á ¤ \  Ò q t|   ¿ º > h_   Œ •“ É r

&

h

“ É r { 9  ô  Ç Y Us $  F g‚  õ   r] X  ) a Y Us $  F g‚  _  0 Au 

\

 ¦    · p  כ s  .  ”  _  Û ¼& 7 ˜à Ô! 3 \ " f _ þ ta Å @Ü ¼– РÒ'  _

  o   © œ\  q Y V l  M :ë  H \  s  ¿ º & h `  ¦ s 6   x 

€

  Û ¼& 7 ˜à Ô! 3 _  y Œ • 0 Au \  @ /6 £ x ÷ &  H  © œ`  ¦ & ñ ½ + É Ã º e ” 



. 7 £ ¤, _ þ ta Å @_  0 Au \  ¦ 0,  r] X  ) a Y Us $  y n C_  spots  e ” 



 H 0 Au \  ¦ 632.8 nm – Ð ¿ º“ ¦ q Y Vd ” `  ¦  6   x €    ) a  . : £ ¤ y

 Û ¼& 7 ˜à Ô! 3 _   ”    « Ñ\  ¦ : Ÿ x K " f  H _ þ ta Å @_  0 Au \  ¦ 

€

Œ

•   H X <  ™ è ™ D ¥1 l x s  e ” `  ¦ % i  9 e ” t ë ß – Y Us $ _   â Ä

º  H  Œ •“ É r spot`  ¦ ë ß –[ þ t l  M :ë  H \  s   ”  `  ¦ s 6   x €   _ þ t a Å

@_  0 Au \  ¦ ~ 1 >  & ñ ½ + É Ã º e ”  . Fig. 4  H Fig. 3 _  Û ¼& 7 ˜ à

Ô! 3   ”  `  ¦ s 6   x # Œ % 3 “ É r Û ¼& 7 ˜à Ô! 3 _   © œZ >  µ 1 ßl  Õ ª A

á Ôs  . Õ ªA á Ô\ " f z  ´‚  “ É r F g " é ¶ _  Û ¼& 7 ˜à Ô! 3 \  _ ô  Ç Õ

ªA á Ôs “ ¦ & h ‚  “ É r Y Us $  c ” \  _ ô  Ç Õ ªA á Ôs  .

D

h– Ðî  r ì  rF g ì  r$ 3  ~ ½ ÓZ O _  & ñ S X ‰$ í õ  Ä »6   x$ í `  ¦  Ž 7 £ x l  0

A # Œ l ^ ‰ ~ ½ ӄ  › ' a \ " f ~ ½ ÓØ  ¦ ÷ &  H y n C_  ì  rF gì  r$ 3 `  ¦ z  ´ r

 % i  . l ^ ‰ ~ ½ ӄ  › ' a Ü ¼– Ѝ  H ² D G ? / õ † < Ɠ §½ ¨ © œ\ " f ×  æ 1

p

x † < Ɠ § z  ´+ « >6   x Ü ¼– Ð ó ø ÍB  “ ¦ e ”   H,  Ø ÔŒ 4 H, à º™ è,  à Ô µ

¢ §, ó ¡ šµ ¢ § ~ ½ ӄ  › ' a`  ¦  6   x % i Ü ¼ 9, ? /Â Ò · ú š§ 4 s   í  H • ¸\ 

› '

a ô  Ç & ñ ˜ Ѝ  H ] j¾ ¡ § õ  † < Êa  ] j/ B N ÷ &t  · ú §€ Œ ¤l  M :ë  H \  · ú ˜ à º e ”

  H ~ ½ ÓZ O “ É r \ O % 3  . Fig. 5 ∼ Fig. 8“ É r Õ ª   õ \  ¦   



· p  כ Ü ¼– Ð Û ¼& 7 ˜à Ô! 3   ”  õ  ì  r$ 3    õ  Õ ªA á Ô\  ¦ 1 l x r \ 



 ? /% 3  .

(5)

Fig. 5. Argon, exposure time 5.0 s.

Fig. 6. Hydrogen, exposure time 4.0 s.

Fig. 7. Sodium, exposure time 1.0 s.

Fig. 8. Helium, exposure time 2.0 s.

Table 1“ É r Û ¼& 7 ˜à Ô! 3 _  peak\  K { © œ   H  © œ, D h– Ðî  r ì

 rF g ì  r$ 3  ~ ½ ÓZ O \  _ K  ½ ¨ô  Ç   õ \  ¦ s  : r ° ú כõ  q “ §ô  Ç ³ ð s

 .  à Ôµ ¢ §, à º™ è, ó ¡ šµ ¢ § _  X <s '   H Jenkins _  F g † < Æ “ § õ

" f [15]\  ¦ ‚ à Л ¸ % i Ü ¼ 9  Ø ÔŒ 4 H l ^ ‰_  s  : r ° ú כ“ É r p 

Table 1. Comparison of experimental peak wavelength with theoretical peak wavelength.

Element

Experimental Theoretical Error Peak(nm) Peak(nm) ratio(%)

Na 586 589 0.5

H

418 410 2.0

470 486 3.3

664 656 1.2

Ar

411 416 1.2

453 451 0.4

499 - -

He 405 - -

²

D G NIST(National Institute of Standards and Technol- ogy) _  X <s ' \  ¦  6   x % i   [16,17]. ³ ð\ " f ˜ Ѝ  H  ü <

° ú

 s  š ¸ Ö  ¦ s  þ j@ / 3.3%s “ ¦ ¨ î ç  H 1.4% – Ð B Ä º ± ú >    M

®

o Ü ¼Ù ¼– Ð s  ~ ½ ÓZ O s  · ú ¡Ü ¼– Ð B Ä º Ä »6   x >   Ö ¸6   x| ¨ c à º e ” 

`

 ¦  כ Ü ¼– Ð l @ /  ) a  .  ë ß –  à Ôµ ¢ § _   â Ä º  H D line s  ì  r K

÷ &t  · ú §€ Œ ¤  H X <, s  כ “ É r ì  rF g l   ^ ‰_  ë  H ] js  9 Æ ÒÊ ê l

> & h “    © œu  > h‚  `  ¦ : Ÿ x K  & ñ x 9 • ¸\  ¦ Z  }{ 9  à º e ” `  ¦  כ Ü ¼

–

Ð ó ø Íé ß –  ) a  . ô  Ǽ # , z  ´+ « >\ " f  H  Ø ÔŒ 4 H _  499 nm, ó ¡ šµ ¢ § _

 405 nm\  K { © œ   H peak  µ 1 Ï| ÷ &% 3 t ë ß – ‚ à Г ¦ « Ñ

\

" f  H K { © œ  © œ_  peak\  ¦ µ 1 Ï| ½ + É Ã º \ O % 3  . s    õ 



 H l ^ ‰~ ½ ӄ  › ' a s  í  H à º >  K { © œ l ^ ‰– Ðë ß – G 0 >t t  · ú §

“

¦ / B N l  1 p x   É r l ^ ‰ Ÿ í† < Ê÷ &% 3 l  M :ë  H“    כ Ü ¼– Ð ó ø Íé ß –

 )

a  . ¿ º t _  l ^ ‰ ™ D ¥ ½ + Ë÷ &# Q e ”   H ~ ½ ӄ  › ' a _  Û ¼& 7 ˜à Ô

! 3

“ É r ¿ º l ^ ‰_  Û ¼& 7 ˜à Ô! 3 s  ×  æ^ o ?÷ &# Q ˜ Ðs l  M :ë  H \  s  ì

 rF g l \  ¦ : Ÿ x K  ~ ½ ӄ  › ' a _  í  H • ¸• ¸ 8 £ ¤& ñ ½ + É Ã º e ”    H & h `  ¦ r

 ô  Ç .

V. + s Ç Â ] Ø õ m Í < gŽ ¹ Å

‘

: r ƒ  ½ ¨\ " f  H @ /› ¸ Û ¼& 7 ˜à Ô! 3   ”  `  ¦ n ”    C  â \ 



_  è  HF K`  ¦ V , `  ¦ € 9 כ ¹ \ O s  Y Us $ \  ¦ s 6   x ô  Ç 8 £ ¤& ñ l ï  r

`

 ¦ 1 l x r \  % 3   H ~ ½ ÓZ O Ü ¼– Ð ç ß –é ß – >  y n C_   © œZ >  Û ¼& 7 ˜à Ô

! 3

`  ¦ ½ ¨   H ~ ½ ÓZ O `  ¦ “ ¦î ß – # Œ l ^ ‰ ~ ½ ӄ  › ' a _  Û ¼& 7 ˜à Ô! 3 

`

 ¦ ì  r$ 3 K  4 Ÿ § Ü ¼– Ð+ ‹ Õ ª ´ òõ \  ¦  Ž 7 £ x % i  . ‘ : r ƒ  ½ ¨\ " f ]

j Œ •ô  Ç ì  rF g ì  r$ 3  r Û ¼% 7 ›“ É r ¨ î ç  H š ¸ Ö  ¦ s  1.4%– Ð & ñ S X ‰

 9 ´ ú §“ É r q 6   x`  ¦ [ þ t s t  · ú §“ ¦ ç ß –é ß – >  ] j Œ •½ + É Ã º e ”  



 H  © œ& h s  e ”  . s  r Û ¼% 7 ›“ É r † < Ɠ §\ " f y n Cõ  Ó ü t| 9 _   © œ  ñ



Œ

•6   x`  ¦ † < Æ_ þ v   H X <• ¸ Ä »6   x  9 y n Cõ  Ò  o¾ ú ˜\  @ /ô  Ç & ñ S X ‰ ô

 Ç > h¥ Æ `  ¦ t >    H † < Æ_ þ v • ¸½ ¨– Ð" f B Ä º Ä »6   x >  s  6

 

x| ¨ c à º e ” `  ¦  כ s  . : £ ¤ y  † < ÆÒ q t[ þ t s  f ” ] X  ì  rF g l \  ¦ ] j Œ •

# Œ z  ´+ « >`  ¦ • ¸2 Ÿ ¤ † < ÊÜ ¼– Ð+ ‹ ^  ¦Ï þ ˜~ à ÌÛ ¼– Ð # Œ t   H ì  r

(6)

F

g l _  1 l x  Œ • " é ¶ o \  ¦ ~ 1 >  s K  • ¸2 Ÿ ¤ • ¸Ö  ¦ à º e ” “ ¦  

«

Ñ\  ¦ % 3 “ ¦ % ƒo    H „   õ & ñ `  ¦  â + « > • ¸2 Ÿ ¤ † < ÊÜ ¼– Ð+ ‹ ë  H ]

jK    0 p x§ 4 `  ¦ ’   © œr ~  ´ à º e ” `  ¦  כ Ü ¼– Ð l @ /  ) a  . Æ ÒÊ ê ì

 rF g l _  ½ ¨› ¸\  ¦  8 > h‚   # Œ & ñ x 9 • ¸\  ¦ Z  } s “ ¦ ¢ ¸ I € ª œ F

g‚  _  á Ô î  r   ñ( ‚  `  ¦ ì  r$ 3    H 1 p x › ' aº   z  ´+ « >`  ¦  € ª œ

>  à º' Ÿ    H Ê ê5 Å q ƒ  ½ ¨\  ¦ : Ÿ x K  Û ¼& 7 ˜à Ô! 3  ì  r$ 3  ~ ½ ÓZ O `  ¦ t

5 Å q& h Ü ¼– Ð > h‚   “ ¦  Ö  ¦  Q D h– Ðî  r ì  rF gì  r$ 3  r Û ¼% 7 ›_ 

 Ö

¸6   x • ¸\  ¦ Z  }{ 9  à º e ” `  ¦  כ Ü ¼– Ð l @ /ô  Ç .

Y

c p w Š à U Ø ”  ô

[1] Philip Sadler, Physic Teacher 29, 423 (1991).

[2] George A. Burman, Overhead Spectroscopy in Ap- paratus for Teaching Physics, edited by Karl C.

Mamola (AAPT, Maryland, 1998), p. 235.

[3] Young-Ae Kim, Eun-Kyeong Lee and Seong-Joo Kang, Journal of the Korean Chemical Society 49, 584 (2005).

[4] Il-Yong Shin, Hyun-Kyung Kim, Byung-Soon Choi, Jong-Yoon Park and Hun-Gi Hong, The Journal of Curriculum and Evaluation 12, 199 (2009).

[5] John H. Moor, Michael A. Coplan and Christopher C. Davis, Building Scientific Apparatus (Addison- Welsley Publishing Company, London, 1983), pp.

222 - 228.

[6] C. Adolf and F. Luis, J. Chem. Educ. 63, 348 (1986).

[7] D. Ulrich and K. Herbert, J. Chem. Educ. 62, 155 (1985).

[8] F. Wakabayashi, K. Hamada and K. Sone, J. Chem.

Educ. 75, 1569 (1998).

[9] F. Wakabayashi and K. Hamada, J. Chem. Educ.

83, 56 (2006).

[10] Edwin Paul Heideman, Film-Canister Spectroscope in Apparatus for Teaching Physics, edited by Karl C. Mamola (AAPT, Maryland, 1998), p. 235.

[11] F. K. Richtmyer, The American Physics Teacher 1, 1 (1933).

[12] Douglas F. Horne, Optical instruments and theier applications (Adam Higger Ltd, Bristol, 1980), pp.

251-254.

[13] Ki-Cheol Park, Sang-Tae Park and Keun-Cheol Yuk, Sae Mulli 52, 497 (2006).

[14] Tae O Seo and Seong-Ryong Ryu, Sae Mulli 58, 171 (2009).

[15] Fransis A. Jenkins and Harvey E. White, Funda- mentals of Optics (McGraw-Hill, New York, 1976), pp. 450 - 453.

[16] http://astro.u-strasbg.fr/∼koppen/discharge/

[17] http://physics.nist.gov/cgi-bin/ASD/lines hold.pl?

el=Ar

수치

Fig. 1. The range of visible spectrum lines; laser spot can be used as a reference.
Fig. 2. Structure of the spectrometer with He-Ne laser as a reference light source.
Fig. 6. Hydrogen, exposure time 4.0 s.

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