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ãå1ãèªé»äœãæ¿å ¥ããå¹³è¡æ¿ã³ã³ãã³ãµã®éé»å®¹é
ç空äžã«ãããŠãäžèŸº $l \text{ [m]}$ ã®æ£æ¹åœ¢é»æ¥µãéé $d \text{ [m]}$ ã§é 眮ããå¹³è¡æ¿ã³ã³ãã³ãµããããå³1ã¯ãã®ã³ã³ãã³ãµã®é»æ¥µæ¿éã«æ¯èªé»ç $\epsilon_r = 5$ ã®èªé»äœãæ¿å ¥ããç¶æ ãå³2ã¯å³1ã®èªé»äœã黿¥µé¢ç©ã® $\frac{1}{2}$ ã ãåŒãåºããç¶æ ã瀺ããŠãããå³1åã³å³2ã®äºã€ã®ã³ã³ãã³ãµã®éé»å®¹é $C_1 \text{ [F]}$ åã³ $C_2 \text{ [F]}$ ã®æ¯ $(C_1 : C_2)$ ãšããŠãæ£ãããã®ã次ã®(1)ïœ(5)ã®ãã¡ããäžã€éžã¹ã
ãã ãã$l \gg d$ ã§ãããã³ã³ãã³ãµã®ç«¯å¹æã¯ç¡èŠã§ãããã®ãšããã

| – | (1) | (2) | (3) | (4) | (5) |
|---|---|---|---|---|---|
| æ¯ ($C_1 : C_2$) | 2 : 1 | 3 : 2 | 5 : 2 | 5 : 3 | 5 : 4 |
解説
æ£è§£ã¯(4)ã§ãã
å¹³è¡æ¿ã³ã³ãã³ãµã®éé»å®¹é $C \text{ [F]}$ ã¯ãèªé»ç $\epsilon \text{ [F/m]}$ã黿¥µé¢ç© $S \text{ [m}^2\text{]}$ãæ¥µæ¿éé $d \text{ [m]}$ ãçšããŠæ¬¡åŒã§è¡šãããŸãã
$$C = \epsilon \frac{S}{d}$$
å³1ã®éé»å®¹é $C_1$ ãæ±ããŸãã黿¥µé¢ç©ã¯ $S = l^2$ ã§ãããæ¯èªé»ç $\epsilon_r = 5$ ã®èªé»äœã§æºããããŠããããã
$$C_1 = \epsilon_r \epsilon_0 \frac{l^2}{d} = 5 \frac{\epsilon_0 l^2}{d} \quad \dots \text{â }$$
å³2ã®éé»å®¹é $C_2$ ãæ±ããŸããèªé»äœãåååŒãåºããç¶æ
ã¯ãé¢ç© $\frac{l^2}{2}$ ã®èªé»äœãããã³ã³ãã³ãµãšãé¢ç© $\frac{l^2}{2}$ ã®çç©ºïŒæ¯èªé»ç1ïŒã®ã³ã³ãã³ãµã䞊åã«æ¥ç¶ãããŠãããšèããŸãã
ããããã®å®¹éã $C_{2a}, C_{2b}$ ãšãããšã
$$C_{2a} (\text{èªé»äœéšå}) = 5 \epsilon_0 \frac{l^2/2}{d} = \frac{5}{2} \frac{\epsilon_0 l^2}{d}$$
$$C_{2b} (\text{ç空éšå}) = 1 \epsilon_0 \frac{l^2/2}{d} = \frac{1}{2} \frac{\epsilon_0 l^2}{d}$$
$$C_2 = C_{2a} + C_{2b} = \left( \frac{5}{2} + \frac{1}{2} \right) \frac{\epsilon_0 l^2}{d} = 3 \frac{\epsilon_0 l^2}{d} \quad \dots \text{â¡}$$
â ãšâ¡ã®æ¯ãæ±ãããšã
$$C_1 : C_2 = 5 : 3$$
ãšãªããŸãã
ãå2ãé»è·ã«åãåã®åæïŒã¯ãŒãã³ã®æ³åïŒ
å³ã®ããã«ãç空äžã® $3 \text{ [m]}$ é¢ãã2ç¹AãBã«ãããã $3 \times 10^{-7} \text{ [C]}$ ã®æ£ã®ç¹é»è·ããããAç¹ãšBç¹ãšãçµã¶ç·åäžã®Aç¹ãã $1 \text{ [m]}$ é¢ããPç¹ã« $Q \text{ [C]}$ ã®æ£ã®ç¹é»è·ã眮ãããšãããã®ç¹é»è·ã«Bç¹ã®æ¹åã« $5 \times 10^{-3} \text{ [N]}$ ã®åãåããããã®ç¹é»è· $Q$ ã®å€ $\text{[C]}$ ãšããŠãæãè¿ããã®ã次ã®(1)ïœ(5)ã®ãã¡ããäžã€éžã¹ã
ãã ããç空äžã®èªé»çã $\epsilon_0 = 8.85 \times 10^{-12} \text{ [F/m]}$ ãšããã

| – | (1) | (2) | (3) | (4) | (5) |
|---|---|---|---|---|---|
| $Q \text{ [C]}$ | $1.2 \times 10^{-9}$ | $1.8 \times 10^{-8}$ | $2.5 \times 10^{-6}$ | $4.4 \times 10^{-5}$ | $7.3 \times 10^{-5}$ |
解説
æ£è§£ã¯(3)ã§ãã
2ã€ã®ç¹é»è·éã«åãéé»å $F \text{ [N]}$ ã¯ãã¯ãŒãã³ã®æ³åã«ããæ¬¡åŒã§æ±ããããŸãã
$$F = k \frac{q_1 q_2}{r^2} = \frac{1}{4 \pi \epsilon_0} \frac{q_1 q_2}{r^2}$$
ããã§ãç空äžã®æ¯äŸå®æ°$k$ã¯ç空äžã®èªé»çã $\epsilon_0 = 8.85 \times 10^{-12} \text{ [F/m]}$ãªã®ã§ä»¥äžã®ããã«æ±ãŸããŸãã
$k \approx 9 \times 10^9 \text{ [N}\cdot\text{m}^2/\text{C}^2\text{]}$ ã䜿çšããŸãã
Pç¹ã«ããç¹é»è· $Q$ ã«åãåãèããŸãã
â Aç¹ã®é»è·ããåããå $F_A$ã¯æ¥åã®ãããBç¹ã®æ¹åã«åããŸããè·é¢ $r_A = 1 \text{ [m]}$ ããã
$$F_A = k \frac{3 \times 10^{-7} \times Q}{1^2} = 3 \times 10^{-7} k Q \text{ [N]}$$
â¡ Bç¹ã®é»è·ããåããå $F_B$ãæ¥åã®ãããAç¹ã®æ¹åã«åããŸããè·é¢ $r_B = 2 \text{ [m]}$ ããã
$$F_B = k \frac{3 \times 10^{-7} \times Q}{2^2} = \frac{3}{4} \times 10^{-7} k Q \text{ [N]}$$
Pç¹ã§ã®åå $F$ ã¯Bç¹æ¹åã« $5 \times 10^{-3} \text{ [N]}$ ãªã®ã§ã $F = F_A – F_B$ ãšãªããŸãã
$$5 \times 10^{-3} = 3 \times 10^{-7} k Q – \frac{3}{4} \times 10^{-7} k Q$$
$$5 \times 10^{-3} = 3 \times 10^{-7} k Q \left( 1 – \frac{1}{4} \right)$$
$$5 \times 10^{-3} = 3 \times 10^{-7} \times (9 \times 10^9) \times Q \times 0.75$$
$$5 \times 10^{-3} = 2025 Q$$
$$Q = \frac{5 \times 10^{-3}}{2025} \approx 2.469 \times 10^{-6} \text{ [C]}$$
æãè¿ãå€ã¯ $2.5 \times 10^{-6}$ ãšãªããŸãã
åèããŒãž

ãå3ãã³ã€ã«ã®èªå·±ã€ã³ãã¯ã¿ã³ã¹
å·»æ° $1000$ ã®ã³ã€ã«ã«çŽæµé»æµ $0.2 \text{ [A]}$ ãæµãããšãã$6 \times 10^{-4} \text{ [Wb]}$ ã®ç£æãçºçããããã®å Žåãã³ã€ã«ã®èªå·±ã€ã³ãã¯ã¿ã³ã¹ $\text{[H]}$ ã®å€ãšããŠãæãè¿ããã®ã次ã®(1)ïœ(5)ã®ãã¡ããäžã€éžã¹ããã ããã³ã€ã«ã®æŒãç£æã¯ç¡èŠã§ãããã®ãšããã
| – | (1) | (2) | (3) | (4) | (5) |
|---|---|---|---|---|---|
| èªå·±ã€ã³ãã¯ã¿ã³ã¹ $\text{[H]}$ | 1 | 2 | 3 | 4 | 5 |
解説
æ£è§£ã¯(3)ã§ãã
èªå·±ã€ã³ãã¯ã¿ã³ã¹ $L \text{ [H]}$ã黿µ $I \text{ [A]}$ãå·»æ° $N$ãç£æ $\Phi \text{ [Wb]}$ ã®éã«ã¯ãç£æé亀æ°ã«é¢ããæ¬¡ã®é¢ä¿ããããŸãã
$$L I = N \Phi$$
ãã®åŒããã $L$ ã«ã€ããŠæ±ãããšã
$$L = \frac{N \Phi}{I}$$
äžããããæ°å€ãä»£å ¥ããŸãã
$$L = \frac{1000 \times 6 \times 10^{-4}}{0.2}$$
$$L = \frac{0.6}{0.2} = 3 \text{ [H]}$$
ãããã£ãŠãèªå·±ã€ã³ãã¯ã¿ã³ã¹ã¯ $3 \text{ [H]}$ ãšãªããŸãã
åèããŒãž

ãå4ãæåœ¢å°ç·ãã€ããäžå¿ã®ç£ç
å³ã®ããã«ãç¹Oãäžå¿ãšããããããååŸ $0.5 \text{ [m]}$ ãšååŸ $1 \text{ [m]}$ ã®å圢å°ç·ã® $\frac{1}{4}$ ã®åŒ§ãããããé£çµããçŽç·ç¶ã®å°ç·ãããªãæåœ¢å°ç·ãããããã®å°ç·ã«ãå³ã«ç€ºãåãã«çŽæµé»æµ $I = 16 \text{ [A]}$ ãæµããå Žåãç¹Oã«ãããç£çã®å€§ãã $H$ ã®å€ $\text{[A/m]}$ ãšããŠãæãè¿ããã®ã次ã®(1)ïœ(5)ã®ãã¡ããäžã€éžã¹ã
ãã ããæåœ¢å°ç·ã¯åäžå¹³é¢äžã«ããããã®å·»æ°ã¯äžå·»ãã§ããããŸããå°ç·ã®å€ªãã¯ç¡èŠã§ãããã®ãšããã

| – | (1) | (2) | (3) | (4) | (5) |
|---|---|---|---|---|---|
| $H \text{ [A/m]}$ | 0.25 | 0.5 | 0.75 | 1.0 | 2.0 |
解説
æ£è§£ã¯(5)ã§ãã
ç¹Oã«ãããç£çã¯ãåå°äœéšåãäœãç£çã®åïŒãã¯ãã«åïŒã§æ±ããããŸããå圢ã³ã€ã«ã®äžå¿ç£ç $H$ ã¯ã $H = \frac{I}{2r} \text{ [A/m]}$ ã§ãã
â ååŸ $r_1 = 0.5 \text{ [m]}$ ã®å匧éšåã¯ãåå šäœã® $\frac{1}{4}$ ãªã®ã§ãç£çã®å€§ãã $H_1$ ã¯ã
$$H_1 = \frac{1}{4} \times \frac{I}{2 r_1} = \frac{1}{4} \times \frac{16}{2 \times 0.5} = 4 \text{ [A/m]}$$
å³ããã®æ³åã«ãããç£çã®åãã¯çŽé¢ã®è£ããè¡šã®æ¹åã§ãã
â¡ ååŸ $r_2 = 1 \text{ [m]}$ ã®å匧éšåãåæ§ã«ãç£çã®å€§ãã $H_2$ ã¯ã
$$H_2 = \frac{1}{4} \times \frac{I}{2 r_2} = \frac{1}{4} \times \frac{16}{2 \times 1} = 2 \text{ [A/m]}$$
黿µã®åãã $r_1$ ã®å匧ãšéã§ãããããç£çã®åãã¯çŽé¢ã®è¡šããè£ã®æ¹åã§ãã
⢠çŽç·éšåã¯ãçŽç·å°äœã®å»¶é·ç·äžã«ç¹OããããããçŽç·éšåã®é»æµãç¹Oã«äœãç£ç㯠$0$ ã§ãã
ãããã£ãŠãç¹Oã«ãããåæç£çã®å€§ãã $H$ ã¯ã
$$H = |H_1 – H_2| = |4 – 2| = 2.0 \text{ [A/m]}$$
ãšãªããŸãã
åèããŒãž

ãå5ãçŽæµåè·¯ã®æ¶è²»é»åã®æ¯èŒ
å³ã®ããã«ãäžã€ã®æµæ $R_1 = 5 \Omega $ã$R_2 = 4 \Omega$ã$R_3 = 8 \Omega$ ãšé»å§ $V \text{ [V]}$ ã®çŽæµé»æºãããªãåè·¯ããããæµæ $R_1, R_2, R_3$ ã®æ¶è²»é»åããããã $P_1 \text{ [W]}, P_2 \text{ [W]}, P_3 \text{ [W]}$ ãšãããšãããã®å€§ããã®å€§ããé ãšããŠãæ£ãããã®ã次ã®(1)ïœ(5)ã®ãã¡ããäžã€éžã¹ã

(1) $P_1 > P_2 > P_3$
(2) $P_1 > P_3 > P_2$
(3) $P_2 > P_1 > P_3$
(4) $P_2 > P_3 > P_1$
(5) $P_3 > P_1 > P_2$
解説
æ£è§£ã¯(1)ã§ãã
åæµæã§ã®æ¶è²»é»åãæ¯èŒããŸããæµæ $R_1$ ãæµããå šé»æµã $I \text{ [A]}$ ãšããŸãã
â æµæ $R_1$ ã®æ¶è²»é»å $P_1$ã«ã€ããŠãå šé»æµ $I$ ãæµããããã
$$P_1 = R_1 I^2 = 5 I^2 \text{ [W]}$$
â¡ æµæ $R_2$ ãš $R_3$ ãžã®é»æµåæµã«ã€ããŠã䞊åéšåã®é»æµã $I_2, I_3$ ãšãããšã黿µã¯æµæã«åæ¯äŸããŠåæµããŸãã
$$I_2 = I \times \frac{R_3}{R_2 + R_3} = I \times \frac{8}{4 + 8} = \frac{2}{3} I \text{ [A]}$$
$$I_3 = I \times \frac{R_2}{R_2 + R_3} = I \times \frac{4}{4 + 8} = \frac{1}{3} I \text{ [A]}$$
â¢ åæµæã®æ¶è²»é»åãèšç®ããŸãã
$$P_2 = R_2 I_2^2 = 4 \times \left( \frac{2}{3} I \right)^2 = \frac{16}{9} I^2 \approx 1.78 I^2 \text{ [W]}$$
$$P_3 = R_3 I_3^2 = 8 \times \left( \frac{1}{3} I \right)^2 = \frac{8}{9} I^2 \approx 0.89 I^2 \text{ [W]}$$
ããããæ¯èŒãããšã $5 I^2 (P_1) > 1.78 I^2 (P_2) > 0.89 I^2 (P_3)$ ãšãªããŸãã
åéžæè¢ãèŠãŠãããŸãã
(1) æ£ãããèšç®ã®çµæã $P_1 > P_2 > P_3$ ãšãªããŸãã
(2) äžæ£è§£ã $P_2$ 㯠$P_3$ ãã倧ãããããé åºãéã§ãã
(3) äžæ£è§£ã $P_1$ ã¯å
šé»æµãæµããããã䞊åéšåã®åé»åãã倧ãããªããŸãã
(4) äžæ£è§£ã $P_1$ ãæå€§ã§ãã
(5) äžæ£è§£ã $P_3$ ã¯æµæå€ã¯å€§ããã§ãããæµãã黿µã $I/3$ ãšå°ãããããé»åã¯æå°ãšãªããŸãã
以äžããã倧ããã®é åºã¯ $P_1 > P_2 > P_3$ ãšãªããŸãã
åèããŒãž


ãå6ã黿± ã®å éšæµæãšèµ·é»å
å³ã®ããã«ãå éšæµæ $r [ \Omega ]$, èµ·é»å $E \text{ [V]}$ ã®é»æ± ã«æµæå€ $R [ \Omega] $ ã®å¯å€æµæåšãæ¥ç¶ããåè·¯ãããã$R = 2.25 \Omega$ ã«ãããšããåè·¯ãæµãã黿µã¯ $I = 3 \text{ A}$ ã§ãã£ããæ¬¡ã«ã$R = 3.45 \Omega$ ã«ãããšããåè·¯ãæµãã黿µã¯ $I = 2 \text{ A}$ ãšãªã£ãããã®é»æ± ã®èµ·é»å $E \text{ [V]}$ ã®å€ãšããŠãæãè¿ããã®ã次ã®(1)ïœ(5)ã®ãã¡ããäžã€éžã¹ã

| – | (1) | (2) | (3) | (4) | (5) |
|---|---|---|---|---|---|
| $E \text{ [V]}$ | 9.30 | 7.20 | 7.05 | 6.90 | 6.75 |
解説
æ£è§£ã¯(2)ã§ãã
黿± ã®å éšæµæ $r$ ãšå¯å€æµæ $R$ ã¯çŽåã«æ¥ç¶ãããŠãããããåè·¯ã®å šæµæã¯ $r + R$ ãšãªããŸãããªãŒã ã®æ³åãããèµ·é»å $E$ 㯠$E = I(r + R)$ ã§è¡šãããŸãã
äžããããäºã€ã®æ¡ä»¶ããé£ç«æ¹çšåŒãç«ãŠãŸãã
$R = 2.25 \Omega$ ã®ãšãã
$E = 3(r + 2.25) \quad \dots \text{â }$
$R = 3.45 \Omega$ ã®ãšãã
$E = 2(r + 3.45) \quad \dots \text{â¡}$
â åŒãšâ¡åŒãç眮ããŠå éšæµæ $r$ ãæ±ããŸãã
$$3(r + 2.25) = 2(r + 3.45)$$
$$3r + 6.75 = 2r + 6.90$$
$$r = 0.15 \Omega$$
ãã®å€ãâ åŒã«ä»£å ¥ã㊠$E$ ãæ±ããŸãã
$$E = 3(0.15 + 2.25) = 3 \times 2.40 = 7.20 \text{ V}$$
ãããã£ãŠã黿± ã®èµ·é»å㯠$7.20 \text{ V}$ ãšãªããŸãã
åèããŒãž

ãå7ãçŽæµåè·¯ã«ãããæµæå€ã®ç®åº
å³ã®ããã«ãå¯å€æµæ $R_1 [\Omega], R_2 [\Omega]$, æµæ $R_x [\Omega]$, 黿º $E \text{ [V]}$ ãããªãçŽæµåè·¯ããããæ¬¡ã«ç€ºãæ¡ä»¶1ã®ãšãã® $R_x [\Omega]$ ã«æµãã黿µ $I \text{ [A]}$ ã®å€ãšæ¡ä»¶2ã®ãšãã®é»æµ $I \text{ [A]}$ ã®å€ã¯çãããªã£ãããã®ãšãã$R_x$ ã®å€ $[\Omega]$ ãšããŠãæãè¿ããã®ã次ã®(1)ïœ(5)ã®ãã¡ããäžã€éžã¹ã
æ¡ä»¶1ïŒ$R_1 = 90 \Omega, R_2 = 6 \Omega$
æ¡ä»¶2ïŒ$R_1 = 70 \Omega, R_2 = 3 \Omega$

| – | (1) | (2) | (3) | (4) | (5) |
|---|---|---|---|---|---|
| $R_x [\Omega]$ | 1.5 | 2.4 | 4.0 | 8.5 | 11.6 |
解説
æ£è§£ã¯(2)ã§ãã
æµæ $R_x$ ã«æµãã黿µ $I$ ã¯ãåè·¯å
šäœã®å
šé»æµ $I_{all}$ ã $R_2$ ãš $R_x$ ã®äžŠåéšåã§åæµãããã®ã§ãã
åè·¯å
šäœã®åææµæ $R_{total} = R_1 + \frac{R_2 R_x}{R_2 + R_x}$ ããã
$$I = \frac{E}{R_1 + \frac{R_2 R_x}{R_2 + R_x}} \times \frac{R_2}{R_2 + R_x} = \frac{E R_2}{R_1(R_2 + R_x) + R_2 R_x}$$
æ¡ä»¶1ã® $I$ ãæ±ããŸãã
$I = \frac{6E}{90(6 + R_x) + 6R_x} = \frac{6E}{540 + 96R_x} \quad \dots \text{â¢}$
æ¡ä»¶2ã® $I$ ãæ±ããŸãã
$I = \frac{3E}{70(3 + R_x) + 3R_x} = \frac{3E}{210 + 73R_x} \quad \dots \text{â£}$
â¢ãšâ£ã®é»æµå€ãçããããã
$$\frac{6}{540 + 96R_x} = \frac{3}{210 + 73R_x}$$
ãããæŽçãããšã
$$2(210 + 73R_x) = 540 + 96R_x$$
$$420 + 146R_x = 540 + 96R_x$$
$$50R_x = 120$$
$$R_x = 2.4 \Omega$$
ãšãªããŸãã
åèããŒãž


ãå8ã亀æµåè·¯ã®é»æµæ¯
å³ã®ããã«ã$R_1 = 20 \Omega$ ãš $R_2 = 30 \Omega$ ã®æµæãéé»å®¹é $C = \frac{1}{100 \pi} \text{ [F]}$ ã®ã³ã³ãã³ãµãã€ã³ãã¯ã¿ã³ã¹ $L = \frac{1}{4 \pi} \text{ [H]}$ ã®ã³ã€ã«ãããªãåè·¯ã«åšæ³¢æ° $f \text{ [Hz]}$ ã§å®å¹å€ $V \text{ [V]}$ ãäžå®ã®äº€æµé»å§ãå ããã$f = 10 \text{ Hz}$ ã®ãšãã« $R_1$ ãæµãã黿µã®å€§ããã $I_{10Hz} \text{ [A]}, f = 10 \text{ MHz}$ ã®ãšãã« $R_1$ ãæµãã黿µã®å€§ããã $I_{10MHz} \text{ [A]}$ ãšããããã®ãšãã黿µæ¯ $\frac{I_{10Hz}}{I_{10MHz}}$ ã®å€ãšããŠãæãè¿ããã®ã次ã®(1)ïœ(5)ã®ãã¡ããäžã€éžã¹ã

| – | (1) | (2) | (3) | (4) | (5) |
|---|---|---|---|---|---|
| 黿µæ¯ | 2.5 | 1.7 | 1.0 | 0.6 | 0.4 |
解説
æ£è§£ã¯(5)ã§ãã
$f = 10 \text{ Hz}$ ã®ãšãã®ãªã¢ã¯ã¿ã³ã¹ãèšç®ãããšã
$X_C = \frac{1}{2 \pi f C} = \frac{1}{2 \pi \times 10 \times \frac{1}{100 \pi}} = 5 \Omega$
$X_L = 2 \pi f L = 2 \pi \times 10 \times \frac{1}{4 \pi} = 5 \Omega$
$X_L = X_C$ ã§ããããã$C$ ãš $L$ ã䞊åã®éšåã¯äžŠåå ±æ¯ãšãªããã€ã³ããŒãã³ã¹ãç¡é倧ãšãªããŸãããããã£ãŠã黿µã¯äžŠåéšåã«ã¯æµãããå路㯠$R_1$ ãš $R_2$ ã®çŽååè·¯ãšã¿ãªããŸãã
$$I_{10Hz} = \frac{V}{R_1 + R_2} = \frac{V}{20 + 30} = \frac{V}{50} \text{ [A]}$$
$f = 10 \text{ MHz}$ ã®ãšããåšæ³¢æ°ãéåžžã«é«ããªããšã$X_C \approx 0$ïŒç絡ïŒã$X_L \approx infty$ïŒéæŸïŒãšãªããŸãããã®ãšã䞊åéšåã¯ççµ¡ç¶æ ãšã¿ãªããããã$R_2$ ã«ã¯é»æµãæµãããå路㯠$R_1$ ã®ã¿ã®åè·¯ãšãªããŸãã
$$I_{10MHz} = \frac{V}{R_1} = \frac{V}{20} \text{ [A]}$$
黿µæ¯ãèšç®ãããš
$$\frac{I_{10Hz}}{I_{10MHz}} = \frac{V/50}{V/20} = \frac{20}{50} = 0.4$$
ãšãªããŸãã
ãå9ã亀æµåè·¯ã®æµæå€ã®ç®åº
å³1ã®ãããªæµæ $R [ \Omega ]$ ãšèªå°æ§ãªã¢ã¯ã¿ã³ã¹ $X [ \Omega ]$ ãšã®çŽååè·¯ãããããã®åè·¯ã«æ£åŒŠæ³¢äº€æµé»å§ $E = 100 \text{ V}$ ãå ãããšããåè·¯ã«æµãã黿µã¯ $10 \text{ A}$ ã§ãã£ãããã®åè·¯ã«å³2ã®ããã«ãæŽã«æµæ $11 \Omega$ ãçŽåæ¥ç¶ãããšãããåè·¯ã«æµãã黿µã¯ $5 \text{ A}$ ã«ãªã£ããæµæ $R [ \Omega ]$ ã®å€ãšããŠãæãè¿ããã®ã次ã®(1)ïœ(5)ã®ãã¡ããäžã€éžã¹ã

| – | (1) | (2) | (3) | (4) | (5) |
|---|---|---|---|---|---|
| $R [ \Omega ]$ | 16.7 | 5.5 | 11.4 | 8.6 | 8.1 |
解説
æ£è§£ã¯(5)ã§ãã
ãªãŒã ã®æ³åãããåç¶æ ã®ã€ã³ããŒãã³ã¹ $Z$ ãæ±ããŸããå³1ã®ç¶æ ã ãš
$Z_1 = \frac{100}{10} = 10 \Omega$
$$R^2 + X^2 = 10^2 = 100 \quad \dots \text{â€}$$
å³2ã®ç¶æ ã ãš
$Z_2 = \frac{100}{5} = 20 \Omega$
$$(R + 11)^2 + X^2 = 20^2 = 400 \quad \dots \text{â¥}$$
â¥åŒãå±éããŸãã
$$R^2 + 22R + 121 + X^2 = 400$$
ãã®åŒã«â€åŒ ($R^2 + X^2 = 100$) ãä»£å ¥ããŸãã
$$100 + 22R + 121 = 400$$
$$22R + 221 = 400$$
$$22R = 179$$
$$R = \frac{179}{22} \approx 8.136 \Omega$$
æãè¿ãå€ã¯ $8.1 \Omega$ ãšãªããŸãã
ãå10ãRLçŽååè·¯ã®éæž¡å¿ç波圢
éæŸé»å§ã $V \text{ [V]}$ ã§åºåæµæãååã«äœãçŽæµé»å§æºãšãã€ã³ãã¯ã¿ã³ã¹ã $L \text{ [H]}$ ã®ã³ã€ã«ãäžããããæµæ $R [ \Omega ]$ ãã¹ã€ãã S ãä»ããŠæ¥ç¶ãããŠãããæå» $t = 0$ ã§ã¹ã€ãã S ãéããã³ã€ã«ã®é»æµ $i_L \text{ [A]}$ ã®æéã«å¯Ÿããå€åãèšæž¬ããã$R = 1 \Omega $ ãšãããšãããæ³¢åœ¢ãå³2ã®ç¹ç·ã®ããã«ãªã£ãã$R = 2 \Omega$ ã§ããã°ã©ã®ãããªæ³¢åœ¢ãšãªãããæ£ãããã®ã次ã®(1)ïœ(5)ã®ãã¡ããäžã€éžã¹ã


解説
æ£è§£ã¯(4)ã§ãã
RLçŽååè·¯ã«ãããŠãã¹ã€ãããéãããšãã®é»æµ $i_L(t)$ ã¯æ¬¡åŒã§è¡šãããŸãã
$$i_L(t) = \frac{V}{R} \left( 1 – e^{-\frac{R}{L}t} \right)$$
æµæ $R$ ã®å€ã $1 \Omega $ ãã $2 \Omega $ ã«å€æŽããéã®å€åã¯ä»¥äžã®éãã§ãã
â å®åžžé»æµïŒæçµå€ïŒã®å€åã«ã€ããŠèããŸããååæéãçµéãããšãã®é»æµå€ã¯ $I = \frac{V}{R}$ ã§ããæµæã2åïŒ$1 \Omega \rightarrow 2 \Omega$ïŒã«ãªããšãå®åžžé»æµã¯ååã«ãªããŸãã
â¡ æå®æ°ã®å€åã«ã€ããŠèããŸããåè·¯ã®æå®æ° $tau$ 㯠$tau = \frac{L}{R}$ ã§ããæµæã2åã«ãªããšãæå®æ°ã¯ååã«ãªããŸããæå®æ°ãå°ãããªãããšã¯ã黿µãå®åžžå€ã«éãããŸã§ã®æéãçããªãïŒç«ã¡äžãããéããªãïŒããšãæå³ããŸãã
ãå11ããã€ãªãŒãã®ç¹æ§ãšçšé
æ¬¡ã®æç« ã¯ãããããã®ãã€ãªãŒãã«ã€ããŠè¿°ã¹ããã®ã§ããã
a. å¯å€å®¹éãã€ãªãŒãã¯ãéä¿¡æ©åšã®å調åè·¯ãªã©ã«çšããããããã®ãã€ãªãŒãã¯ãpnæ¥åã« (ã¢) é»å§ãå ããŠäœ¿çšãããã®ã§ããã
b. pnæ¥åã« (ã€) é»å§ãå ãããã®å€ã倧ããããŠãããšãéäŒçŸè±¡ãèµ·ããããã®éäŒé»å§ä»è¿ã§ã¯ãæµãã黿µãå€åããŠãæ¥å䞡端ã®é»å§ã¯ã»ãŒäžå®ã«ä¿ããããå®é»å§ãã€ãªãŒãã¯ããã®æ§è³ªãå©çšããŠæå®ã®å®é»å§ãåŸãããã«ã€ãããããã€ãªãŒãã§ããã
c. ã¬ãŒã¶ãã€ãªãŒãã¯å éä¿¡ãå æ å ±æ©åšã®å æºãšããŠå©çšãããpnæ¥åã« (ãŠ) é»å§ãå ããŠäœ¿çšãããã®ã§ããã
äžèšã®èšè¿°äžã®ç©ºçœç®æ(ã¢)ïœ(ãŠ)ã«åœãŠã¯ãŸãèªå¥ãšããŠãæ£ãããã®ãçµã¿åãããã®ã¯æ¬¡ã®ãã¡ã©ããã
| – | (ã¢) | (ã€) | (ãŠ) |
|---|---|---|---|
| (1) | é æ¹å | é æ¹å | éæ¹å |
| (2) | éæ¹å | éæ¹å | é æ¹å |
| (3) | éæ¹å | é æ¹å | éæ¹å |
| (4) | é æ¹å | éæ¹å | é æ¹å |
| (5) | éæ¹å | éæ¹å | éæ¹å |
解説
æ£è§£ã¯(2)ã§ãã
åãã€ãªãŒãã®åäœåçãšãã€ã¢ã¹æ¹åã¯ä»¥äžã®éãã§ãã
(ã¢) å¯å€å®¹éãã€ãªãŒãïŒããªãã£ããïŒã¯ãpnæ¥åã«éæ¹åé»å§ãããããšãé»å§ã®å€§ããã«å¿ããŠç©ºä¹å±€ã®åããå€åããéé»å®¹éãå€åããæ§è³ªãå©çšããŸãã
(ã€) å®é»å§ãã€ãªãŒãïŒãã§ããŒãã€ãªãŒãïŒã¯ãpnæ¥åã«éæ¹åé»å§ããããç¹å®ã®é»å§ïŒéäŒé»å§ïŒã§æ¥æ¿ã«é»æµãæµããéäŒçŸè±¡ãå©çšããŠãé»å§ãäžå®ã«ä¿ã¡ãŸãã
(ãŠ) ã¬ãŒã¶ãã€ãªãŒã: pnæ¥åã«é æ¹åé»å§ãæµããæ³šå ¥ããããã£ãªã¢ãåçµåããéã«å ãæŸåºïŒèªå°æŸåºïŒããåçãå©çšããŠããŸãã
ãã£ãŠãåéžæè¢ã®æ£åŠã¯ä»¥äžã®ãšããã
(1) aãé æ¹åãšãªã£ãŠãããã誀ãã
(2) æ£ãããå
šãŠã®çµã¿åãããåèŽããŠããŸãã
(3) bãé æ¹åãšãªã£ãŠãããã誀ãã
(4) aãé æ¹åãcãéæ¹åãšãªã£ãŠãããã誀ãã
(5) cãéæ¹åãšãªã£ãŠãããã誀ãã
ãå12ãé»çäžã®é»åã®éå
å³ã®ããã«ãç空äžã«é»æ¥µéé $d \text{ [m]}$ ã®å¹³è¡æ¿é»æ¥µããããé°æ¥µæ¿äžã«é»åã眮ãããéœæ¥µæ¿ã«é»å§ $V \text{ [V]}$ ãå ãããšãããã®é»åã«å ããå $F \text{ [N]}$ ã®åŒãšããŠãæ£ããã®ã¯æ¬¡ã®ãã¡ã©ããã
ãã ããé»åã®è³ªéã $m \text{ [kg]}$ã黿°çŽ éã $e \text{ [C]}$ ãšããããŸãã黿¥µæ¿ã®ç«¯å¹æã¯ç¡èŠã§ãããã®ãšããã

(1) $\frac{V}{d}e$
(2) $\frac{V}{d^2}e$
(3) $\frac{V}{d^2} \frac{m}{e}$
(4) $\frac{V}{d^2} em$
(5) $\frac{V^2}{d} e$
解説
æ£è§£ã¯(1)ã§ãã
å¹³è¡æ¿é»æ¥µéã«é»å§ $V$ [V] ãå ãããšã黿¥µéã«ã¯äžæ§ãªé»ç $E$ [V/m] ãçããŸããé»çã®å€§ããã¯æ¬¡åŒã§è¡šãããŸãã
$$E = \frac{V}{d} \quad [\text{V/m}]$$
ãã®é»çäžã«ããé»è· $q$ [C] ãåããéé»å $F$ [N] ã¯ã $F = qE$ ã§ããé»åã®é»è·ïŒçµ¶å¯Ÿå€ïŒã¯é»æ°çŽ é $e$ [C] ã§ãããããä»£å ¥ãããšæ¬¡åŒã®ããã«ãªããŸãã
$$F = eE = e \left( \frac{V}{d} \right) = \frac{V}{d}e \quad [\text{N}]$$
ãããã£ãŠãåŒ(1)ãæ£è§£ãšãªããŸããé»åã®è³ªé $m$ ã¯å éåºŠãæ±ããéã«ã¯å¿ èŠã§ãããé»åã«å ãããåããã®ãã®ã®åŒã«ã¯å«ãŸããŸããã
ãå13ãæ°Žæ¶æ¯ååãšæ°Žæ¶çºæ¯åè·¯
æ°Žæ¶æ¯ååãšæ°Žæ¶çºæ¯åè·¯ã«é¢ããèšè¿°ãšããŠã誀ã£ãŠãããã®ã次ã®(1)ïœ(5)ã®ãã¡ããäžã€éžã¹ã
(1) æ°Žæ¶æ¯ååã¯ãæ°Žæ¶çãäºã€ã®é»æ¥µã§æãã çŽ åã§ããã
(2) æ°Žæ¶æ¯ååã®é»æ°çãªç䟡åè·¯ã«ã¯ãçŽåå
±æ¯åšæ³¢æ°ãšäžŠåå
±æ¯åšæ³¢æ°ã®å·®ãéåžžã«å°ãããšããç¹åŸŽãããã
(3) æ°Žæ¶çºæ¯åè·¯ã¯ãLC çºæ¯åè·¯ã®ã³ã³ãã³ãµãæ°Žæ¶æ¯ååã«çœ®ãæãããã®ã§ããã
(4) æ°Žæ¶çºæ¯åè·¯ã¯ãLC çºæ¯åè·¯ãšæ¯èŒããŠåšæ³¢æ°å€åãéåžžã«å°ããã
(5) æ°Žæ¶çºæ¯åè·¯ãçšããåšæ³¢æ°ã·ã³ã»ãµã€ã¶ã¯ãç¡ç·éä¿¡æ©ã®åšæ³¢æ°æºãšããŠå©çšãããŠããã
解説
誀ã£ãŠããã®ã¯(3)ã§ãã
åéžæè¢ã®è§£èª¬ã¯ä»¥äžã®éãã§ãã
(1) æ£ãããæ°Žæ¶æ¯ååã¯ã人工氎æ¶ãªã©ã®æ°Žæ¶çã®äž¡é¢ã«é»æ¥µãåãä»ããæ§é ãããŠããŸãã
(2) æ£ãããæ°Žæ¶æ¯ååã¯éåžžã«é«ãQïŒåè³ªä¿æ°ïŒãæã¡ãçŽåå
±æ¯åšæ³¢æ° $f_s$ ãšäžŠåå
±æ¯åšæ³¢æ° $f_p$ ãæ¥µããŠæ¥è¿ããŠããã®ãç¹åŸŽã§ãã
(3) 誀ããæ°Žæ¶æ¯ååã¯ç¹å®ã®åšæ³¢æ°ç¯å²ã§èªå°æ§ïŒã³ã€ã«ã®æ§è³ªïŒã瀺ããããäžè¬çã«ã¯LCçºæ¯åè·¯ã®ã³ã€ã«ïŒã€ã³ãã¯ã¿ã³ã¹ïŒã®ä»£ããã«ããããã¯å
±æ¯åè·¯ã®äžéšãšããŠçµã¿èŸŒãŸããŸããã³ã³ãã³ãµã眮ãæãããã®ãšããèšè¿°ã¯äžé©åã§ãã
(4) æ£ãããæ°Žæ¶æ¯ååã®å
±æ¯ç¹æ§ã¯éåžžã«éããããåšå²ã®æž©åºŠå€åãªã©ã«ããåšæ³¢æ°ã®å€åãLCåè·¯ã«æ¯ã¹ãŠæ¥µããŠå°ãããå®å®ããçºæ¯ãå¯èœã§ãã
(5) æ£ãããé«ãåšæ³¢æ°å®å®æ§ãæ±ããããç¡ç·æ©ã®åºæºåšæ³¢æ°æºãšããŠãæ°Žæ¶çºæ¯åšã¯åºãå©çšãããŠããŸãã
ãå14ãå šæ³¢æŽæµåœ¢é»å§èšã«ããæž¬å®
ç®çãæ£åŒŠæ³¢äº€æµã«å¯Ÿããå®å¹å€ã«ãªãæŽæµåœ¢ã®é»å§èš(å šæ³¢æŽæµåœ¢)ãããããã®é»å§èšã§å³ã®ãããªåšæ $20 \text{ ms}$ ã®ç¹°ãè¿ã波圢é»å§ã枬å®ããããã®ãšããé»å§èšã®æç€ºã®å€ $\text{[V]}$ ãšããŠãæãè¿ããã®ã次ã®(1)ïœ(5)ã®ãã¡ããäžã€éžã¹ã

| – | (1) | (2) | (3) | (4) | (5) |
|---|---|---|---|---|---|
| æç€ºå€ [V] | 5.66 | 5.14 | 4.62 | 4.44 | 4.00 |
解説
æ£è§£ã¯(4)ã§ãã
æŽæµåœ¢é»å§èšïŒå šæ³¢æŽæµåœ¢ïŒã¯ãå ¥åãããæ³¢åœ¢ã®çµ¶å¯Ÿå¹³åå€ $V_{avg_abs}$ ãæ€åºãããããæ£åŒŠæ³¢ã®å®å¹å€ $V_{rms_sine}$ ã«æç®ããŠè¡šç€ºããèšåšã§ããæ£åŒŠæ³¢ã«ãããŠãå®å¹å€ / å¹³åå€ãã®æ¯ïŒæ³¢åœ¢çïŒã¯çŽ $1.11$ ãªã®ã§ãèšåšã®æç€ºå€ $V_{ind}$ ã¯æ¬¡åŒã§æ±ããããŸãã
$$V_{ind} = 1.11 \times V_{avg_abs}$$
â å ¥åæ³¢åœ¢ã®çµ¶å¯Ÿå¹³åå€ãæ±ããŸããå³ã®æ³¢åœ¢ã¯åšæ $T = 20 \text{ ms}$ ã§ããã $0$ ïœ $10 \text{ ms}$ ã§ $8 \text{ V}$ ã $10$ ïœ $20 \text{ ms}$ ã§ $0 \text{ V}$ ãªã®ã§ã1åšæã®å¹³åå€ã¯ä»¥äžã®éãã§ãã
$$V_{avg_abs} = \frac{1}{20} \int_{0}^{20} |v(t)| dt = \frac{1}{20} (8 \times 10 + 0 \times 10) = 4 \text{ V}$$
â¡ èšåšã®æç€ºå€ãæ±ããŸããæ£åŒŠæ³¢ç®çã®æç®ä¿æ° $1.11$ ãä¹ããŸãã
$$V_{ind} = 1.11 \times 4 = 4.44 \text{ V}$$
ãããã£ãŠã(4)ã®å€ãæãè¿ããªããŸãã
ãå15ãäžçžäº€æµåè·¯ã®èšç®
å³ã®ããã«ç·éé»å§ $200 \text{ V}$ãåšæ³¢æ° $50 \text{ Hz}$ ã®å¯Ÿç§°äžçžäº€æµé»æºã« RLC è² è·ãæ¥ç¶ãããŠããã $R = 10 \text{ \Omega}$ã黿ºè§åšæ³¢æ°ã $\Omega \text{ [rad/s]}$ ãšããŠã $\Omega L = 20 [ \Omega ]$ã $\frac{1}{\Omega C} = 20 \text{ \Omega}$ ã§ãããæ¬¡ã®(a)åã³(b)ã®åã«çããã

(a) 黿ºé»æµ $I \text{ [A]}$ ã®å€ãšããŠãæãè¿ããã®ã次ã®(1)ïœ(5)ã®ãã¡ããäžã€éžã¹ã
(1) 5.77 (2) 7.00 (3) 11.5 (4) 14.0 (5) 22.5
(b) äžçžè² è·ã®æå¹é»å $P \text{ [kW]}$ ã®å€ãšããŠãæãè¿ããã®ã次ã®(1)ïœ(5)ã®ãã¡ããäžã€éžã¹ã
(1) 2.6 (2) 1.3 (3) 4.0 (4) 3.5 (5) 12
解説
æ£è§£ã¯(a)ã(3)ã(b)ã(3)ã§ãã
å³ã®äžçžè² è·ã¯ã¹ã¿ãŒïŒYïŒçµç·ã§ãããåçžã«æµæ $R$ãã³ã€ã« $L$ãã³ã³ãã³ãµ $C$ ã䞊åã«æ¥ç¶ãããŠããŸãã
(a) 1çžåã®é»æµãæ±ããŸãã
çžé»å§ $V_p$ ã¯ãç·éé»å§ $V = 200 \text{ V}$ ããæ¬¡ã®ããã«æ±ããããŸãã
$$V_p = \frac{200}{sqrt{3}} \approx 115.5 \text{ V}$$
åçŽ åãæµãã黿µ $I_R, I_L, I_C$ ã¯ä»¥äžã®éãã§ãã
$I_R = \frac{V_p}{R} = \frac{115.5}{10} = 11.55 \text{ A}$
$I_L = \frac{V_p}{\Omega L} = \frac{115.5}{20} \approx 5.78 \text{ A}$
$I_C = \frac{V_p}{1/(\Omega C)} = \frac{115.5}{20} \approx 5.78 \text{ A}$
ã³ã€ã«ã®é»æµãšã³ã³ãã³ãµã®é»æµã¯äœçžã $180^circ$ ç°ãªãããã䞊åéšåã®ç¡å¹é»æµ $I_X$ 㯠$I_X = |I_L – I_C| = 0 \text{ A}$ ãšãªããŸãïŒäžŠåå
±æ¯ç¶æ
ïŒã
ãã£ãŠã黿ºé»æµïŒçžé»æµïŒ $I$ ã¯æµæãæµãã黿µæåã®ã¿ãšãªãã $I = I_R = 11.55 \text{ A}$ ã§ããæãè¿ãå€ã¯ $11.5$ ãšãªããŸãã
(b) äžçžã®æå¹é»å $P$ ãæ±ããŸããæå¹é»åã¯æµæã®ã¿ã§æ¶è²»ãããŸãã
$$P = 3 \times V_p I_R = 3 \times \frac{200}{sqrt{3}} \times 11.55 \approx 3 \times \frac{40000/3}{10} = 4000 \text{ W}$$
ãŸã㯠$P = sqrt{3} V I cos theta$ ãããå ±æ¯ã«ãã $cos theta = 1$ ã®ããã
$$P = sqrt{3} \times 200 \times 11.55 \approx 1.732 \times 200 \times 11.55 \approx 4000 \text{ W} = 4.0 \text{ kW}$$
ãã£ãŠãæãè¿ãå€ã¯ $4.0$ ãšãªããŸãã
ãå16ãçŽæµããªããžåè·¯ã®èšç®
å³ã®çŽæµåè·¯ã«ãããŠã次ã®(a)åã³(b)ã«çããããã ãã黿ºé»å§ $E \text{ [V]}$ ã®å€ã¯äžå®ã§å€åããªããã®ãšããã

(a) å³1ã®ããã«æµæ $R \text{ [\Omega]}$ ã端å a, d éã«æ¥ç¶ãããšãã $I_1 = 4.5 \text{ A}$ã $I_2 = 0.5 \text{ A}$ ã®é»æµãæµãããæµæ $R$ ã®å€ $[ \Omega ]$ ãšããŠãæ£ãããã®ã次ã®(1)ïœ(5)ã®ãã¡ããäžã€éžã¹ã
(1) 180 (2) 160 (3) 80 (4) 40 (5) 20
(b) å³1ã®æµæ $R [ \Omega ]$ ãå³2ã®ããã«ç«¯å b, c éã«æ¥ç¶ãçŽãããšããåè·¯ã«æµãã黿µ $I_3$ ã®å€ $\text{[A]}$ ãšããŠãæãè¿ããã®ã次ã®(1)ïœ(5)ã®ãã¡ããäžã€éžã¹ã
(1) 5.5 (2) 4.8 (3) 4.5 (4) 4.2 (5) 4.0
解説
æ£è§£ã¯(a)ã(3)ã(b)ã(4)ã§ãã
(a) å³1ã«ãããŠã端å a-b-d éããã³ a-c-d éã®åæè·¯ã®æµæã¯ $16 + 4 = 20 \Omega$ ã§ãã
äžŠåæ¥ç¶ããã2ã€ã®æè·¯ã®åææµæ $R_{abc}$ 㯠$10 \Omega$ ã§ãããããã«é»æµ $I_{arm} = (I_1 – I_2) / 2 = (4.5 – 0.5) / 2 = 2 \text{ A}$ ãæµããŠããŸãã
黿ºé»å§ $E$ ã¯
$E = R_{arm} I_{arm} = 20 \times 2 = 40 \text{ V}$
ã§ããæµæ $R$ ã«ã¯é»æµ $I_2 = 0.5 \text{ A}$ ãæµããŠããããã
$$R = \frac{E}{I_2} = \frac{40}{0.5} = 80 \text{ \Omega}$$
(b) å³2ã®åè·¯ã¯ããªããžåè·¯ã§ãããç©ã®å¯ŸèŸºïŒ$16 \times 16 neq 4 \times 4$ïŒãçãããªããã平衡ããŠããŸããã
$Delta-Y$ 倿çãçšããŠåè·¯ãæŽçãããšãå
šé»æµ $I_3$ ã¯çŽ $4.17 \text{ A}$ ãšæ±ããããŸãã
æãè¿ãå€ã¯ $4.2$ ã§ãã
ãå17ãè€åèªé»äœã³ã³ãã³ãµã®é»çãšãšãã«ã®ãŒ
å³ã®ããã«ã極æ¿éã®åã $d \text{ [m]}$ã衚é¢ç© $S \text{ [m}^2\text{]}$ ã®å¹³è¡æ¿ã³ã³ãã³ãµAãšBããããç空ã®èªé»çã $\epsilon_0 \text{ [F/m]}$ ãšãããäž¡ã³ã³ãã³ãµã®äžåŽã®æ¥µæ¿ã«é»å§ $V \text{ [V]}$ ãæ¥ç¶ãããæ¬¡ã®(a)åã³(b)ã®åã«çããã

(a) ã³ã³ãã³ãµAã«ãããåèªé»äœå
éšã®é»çã®åŒ·ã $E_{A1}, E_{A2}, E_{A3}$ ã®å€§å°é¢ä¿ãšãã®äžã®æå€§å€ã®çµåããšããŠãæ£ãããã®ã次ã®(1)ïœ(5)ã®ãã¡ããäžã€éžã¹ã
(1) $E_{A1} < E_{A2} < E_{A3}, \quad \frac{3V}{5d}$
(2) $E_{A1} > E_{A2} > E_{A3}, \quad \frac{3V}{5d}$
(3) $E_{A1} = E_{A2} = E_{A3}, \quad \frac{V}{d}$
(4) $E_{A1} < E_{A2} < E_{A3}, \quad \frac{9V}{5d}$
(5) $E_{A1} > E_{A2} > E_{A3}, \quad \frac{9V}{5d}$
(b) ã³ã³ãã³ãµBå
šäœã®èç©ãšãã«ã®ãŒã¯ãã³ã³ãã³ãµAå
šäœã®èç©ãšãã«ã®ãŒã®äœåããæãè¿ããã®ã次ã®(1)ïœ(5)ã®ãã¡ããäžã€éžã¹ã
(1) 0.72 (2) 0.83 (3) 1.00 (4) 1.20 (5) 1.38
解説
æ£è§£ã¯(a)ã(5)ã(b)ã(4)ã§ãã
(a) ã³ã³ãã³ãµAã¯3å±€ã®çŽåæ¥ç¶ã§ããçŽåæ¥ç¶ã§ã¯é»æå¯åºŠ $D$ ãäžå®ïŒ$D_1 = D_2 = D_3$ïŒã§ãããé»ç $E$ 㯠$E = D / \epsilon$ ããæ¯èªé»çã«åæ¯äŸããŸããæ¯èªé»ç㯠$2\epsilon_0, 3\epsilon_0, 6\epsilon_0$ ãšäžå±€ã»ã©å€§ãããããé»çã®åŒ·ãã¯äžå±€ã»ã©å€§ããã $E_{A1} > E_{A2} > E_{A3}$ ãšãªããŸããæå€§é»ç $E_{A1}$ ãæ±ãããšãé»å§ã®é¢ä¿åŒãã $E_{A1} = \frac{9V}{5d}$ ãšå°ãããŸãã
(b) åã³ã³ãã³ãµã®åæéé»å®¹é $C_A, C_B$ ãæ±ããŸããèç©ãšãã«ã®ãŒ $W$ 㯠$W = \frac{1}{2} C V^2$ ã§è¡šãããŸããèšç®ã®çµæã $C_B$ 㯠$C_A$ ã® $1.2$ åãšãªãããããšãã«ã®ãŒã $1.20$ åãšãªããŸãã
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解説
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