MCP๋กœ ์—ฐ๊ฒฐ โ†’

๊ณ„์‚ฐ ์ž…๋ ฅ

๊ณต์‹

๊ด‘๊ณ 

๊ฒฐ๊ณผ

ํ€ด๋ฆฌ ์ƒ์ˆ˜
20,764.8905
Kยทmยณ  (ฯ‡ = C / T)
์ˆ˜๋ฐ€๋„ N 10,000,000,000,000,000,000,000,000,000 mโปยณ
์ž๊ธฐ ๋ชจ๋ฉ˜ํŠธ ฮผ 0 J/T
๋ณผ์ธ ๋งŒ ์ƒ์ˆ˜ k_B 0 J/K

ํ€ด๋ฆฌ ์ƒ์ˆ˜๋ž€?

ํ€ด๋ฆฌ ์ƒ์ˆ˜(C)๋Š” ์ƒ์ž์„ฑ์— ๊ด€ํ•œ ํ€ด๋ฆฌ ๋ฒ•์น™์— ๋“ฑ์žฅํ•˜๋Š” ๋ฌผ์งˆ ๊ณ ์œ ์˜ ๊ฐ’์ž…๋‹ˆ๋‹ค. ํ€ด๋ฆฌ ๋ฒ•์น™์€ ์ƒ์ž์„ฑ์ฒด์˜ ์ž๊ธฐ ๊ฐ์ˆ˜์œจ์ด ์˜จ๋„์— ๋ฐ˜๋น„๋ก€ํ•œ๋‹ค๋Š” ๊ฒƒ์„ ๋งํ•˜๋ฉฐ, ์‹์œผ๋กœ ๋‚˜ํƒ€๋‚ด๋ฉด \(\chi = C / T\)์ž…๋‹ˆ๋‹ค. ์ด ์ƒ์ˆ˜๋Š” ์ž๊ธฐ ๋ชจ๋ฉ˜ํŠธ์˜ ๋ฐ€๋„์™€ ๊ฐ ๋ชจ๋ฉ˜ํŠธ์˜ ํฌ๊ธฐ์— ๋”ฐ๋ผ ๊ฒฐ์ •๋ฉ๋‹ˆ๋‹ค. ์ด ๊ณ„์‚ฐ๊ธฐ๋Š” ํŠน์ • ๊ตญ๊ฐ€์— ํ•œ์ •๋˜์ง€ ์•Š๋Š” ๋ณดํŽธ์ ์ธ ๋ฌผ๋ฆฌ ๋„๊ตฌ๋กœ, ์–ด๋””์„œ๋‚˜ ์ ์šฉ๋˜๋ฉฐ ์ „ ๊ณผ์ •์—์„œ SI ๋‹จ์œ„๋ฅผ ์‚ฌ์šฉํ•ฉ๋‹ˆ๋‹ค.

Curie law graph showing susceptibility decreasing with temperature and inverse susceptibility rising linearly
The Curie law: susceptibility ฯ‡ falls as 1/T, so the inverse 1/ฯ‡ is a straight line whose slope is set by the Curie constant.

๊ณ„์‚ฐ๊ธฐ ์‚ฌ์šฉ๋ฒ•

์„ธ ๊ฐ€์ง€ ๊ฐ’์„ ์ž…๋ ฅํ•˜์„ธ์š”. ์ž๊ธฐ ๋ชจ๋ฉ˜ํŠธ์˜ ์ˆ˜๋ฐ€๋„ \(N\)(์„ธ์ œ๊ณฑ๋ฏธํ„ฐ๋‹น ๋ชจ๋ฉ˜ํŠธ ๊ฐœ์ˆ˜), ๊ฐ ์ž…์ž์˜ ์œ ํšจ ์ž๊ธฐ ๋ชจ๋ฉ˜ํŠธ \(\mu\)(ํ…Œ์Šฌ๋ผ๋‹น ์ค„, J/T), ๊ทธ๋ฆฌ๊ณ  ๋ณผ์ธ ๋งŒ ์ƒ์ˆ˜ \(k_B\)(์ •ํ™•ํ•œ SI ๊ฐ’ \(1.380649 \times 10^{-23}\) J/K๊ฐ€ ๋ฏธ๋ฆฌ ์ž…๋ ฅ๋˜์–ด ์žˆ์Šต๋‹ˆ๋‹ค). ๊ณ„์‚ฐ ๋ฒ„ํŠผ์„ ๋ˆ„๋ฅด๋ฉด Kยทmยณ ๋‹จ์œ„์˜ ํ€ด๋ฆฌ ์ƒ์ˆ˜๋ฅผ ์–ป์„ ์ˆ˜ ์žˆ์œผ๋ฉฐ, ์ด ๊ฐ’์€ ๊ณง๋ฐ”๋กœ \(\chi = C/T\) ์‹์— ๋Œ€์ž…ํ•  ์ˆ˜ ์žˆ์Šต๋‹ˆ๋‹ค.

๊ณต์‹ ํ’€์ด

ํ€ด๋ฆฌ ์ƒ์ˆ˜๋Š” ๋‹ค์Œ๊ณผ ๊ฐ™์ด ์ฃผ์–ด์ง‘๋‹ˆ๋‹ค.

$$C = \frac{N \cdot \mu^{2}}{3 \cdot k_B}$$

์—ฌ๊ธฐ์„œ \(N \cdot \mu^2\)๋Š” ๋‹จ์œ„ ๋ถ€ํ”ผ๋‹น ์ „์ฒด ์ž๊ธฐ ์‘๋‹ต์„ ๋‚˜ํƒ€๋‚ด๊ณ , ์ธ์ž 3์€ 3์ฐจ์› ๊ณต๊ฐ„์˜ ๋ชจ๋“  ๋ฐฉํ–ฅ์— ๋Œ€ํ•ด ๋ชจ๋ฉ˜ํŠธ์˜ ๋ฐฉํ–ฅ์„ ํ‰๊ท ๋‚ธ ๋ฐ์„œ ๋‚˜์˜ต๋‹ˆ๋‹ค. ๊ทธ๋ฆฌ๊ณ  ์—ด์—๋„ˆ์ง€ ์ฒ™๋„์ธ \(k_B\)๋กœ ๋‚˜๋ˆ„์–ด ๋ชจ๋ฉ˜ํŠธ์˜ ์ •๋ ฌ๊ณผ ์˜จ๋„๋ฅผ ์—ฐ๊ฒฐํ•ฉ๋‹ˆ๋‹ค. ๋ชจ๋ฉ˜ํŠธ๊ฐ€ ํฌ๊ฑฐ๋‚˜ ๋ฐ€๋„๊ฐ€ ๋†’์„์ˆ˜๋ก \(C\)๋Š” ์ปค์ง€๊ณ , ์—ด์  ์š”๋™(\(k_B\))์ด ํด์ˆ˜๋ก \(C\)๋Š” ์ž‘์•„์ง‘๋‹ˆ๋‹ค.

Array of randomly oriented magnetic moment arrows representing paramagnetic dipoles in a field
Paramagnetism arises from many magnetic moments ฮผ that partly align with an external field H.

๊ณ„์‚ฐ ์˜ˆ์‹œ

์˜ˆ๋ฅผ ๋“ค์–ด \(N = 1 \times 10^{28}\) ๊ฐœ/mยณ, \(\mu = 9.274 \times 10^{-24}\) J/T(์•ฝ ๋ณด์–ด ๋งˆ๊ทธ๋„คํ†ค 1๊ฐœ)์ด๋ผ๊ณ  ํ•ฉ์‹œ๋‹ค. ๊ทธ๋Ÿฌ๋ฉด \(\mu^2 = 8.6007 \times 10^{-47}\), \(N \cdot \mu^2 = 8.6007 \times 10^{-19}\)์ด ๋˜๊ณ , ์ด๋ฅผ \(3 \cdot k_B = 4.141947 \times 10^{-23}\)๋กœ ๋‚˜๋ˆ„๋ฉด ๋‹ค์Œ์„ ์–ป์Šต๋‹ˆ๋‹ค.

$$C \approx 2.0765 \times 10^{4} \ \text{K}\cdot\text{m}^3$$

์ด๋ ‡๊ฒŒ ๊ตฌํ•œ ๊ฐ’์œผ๋กœ ์ž„์˜์˜ ์˜จ๋„์—์„œ์˜ ๊ฐ์ˆ˜์œจ์„ \(\chi = C/T\)๋กœ ์˜ˆ์ธกํ•  ์ˆ˜ ์žˆ์Šต๋‹ˆ๋‹ค.

์ž์ฃผ ๋ฌป๋Š” ์งˆ๋ฌธ

์–ด๋–ค ๋‹จ์œ„๋ฅผ ์‚ฌ์šฉํ•˜๋‚˜์š”? ์—„๊ฒฉํ•œ SI ๋‹จ์œ„์ž…๋‹ˆ๋‹ค. \(N\)์€ \(\text{m}^{-3}\), \(\mu\)๋Š” J/T, \(k_B\)๋Š” J/K์ด๋ฉฐ, ๊ทธ ๊ฒฐ๊ณผ \(C\)๋Š” Kยทmยณ ๋‹จ์œ„๋กœ ๋‚˜์˜ต๋‹ˆ๋‹ค.

์œ ํšจ ์ž๊ธฐ ๋ชจ๋ฉ˜ํŠธ๋ž€ ๋ฌด์—‡์ธ๊ฐ€์š”? ์ด์˜จ์˜ ๊ฒฝ์šฐ \(\mu = g \cdot \sqrt{J(J+1)} \cdot \mu_B\)๋กœ ์ฃผ์–ด์ง€๋ฉฐ, ์—ฌ๊ธฐ์„œ \(\mu_B = 9.274 \times 10^{-24}\) J/T๋Š” ๋ณด์–ด ๋งˆ๊ทธ๋„คํ†ค์ž…๋‹ˆ๋‹ค.

์™œ 3์œผ๋กœ ๋‚˜๋ˆ„๋‚˜์š”? ์ธ์ž 3์€ 3์ฐจ์›์—์„œ ์ธ๊ฐ€ ์ž๊ธฐ์žฅ ๋ฐฉํ–ฅ์œผ๋กœ ํˆฌ์˜๋œ ๋ชจ๋ฉ˜ํŠธ์˜ ๋ฐฉํ–ฅ(์—ด์ ) ํ‰๊ท ์—์„œ ๋น„๋กฏ๋ฉ๋‹ˆ๋‹ค.

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