Problem 15.1 Challenge
หัวข้อ: กฎของบิโอต์–ซาวาร์ต (The Biot – Savart Law)
\(\vec{B} =\frac{\mu _{0}I}{4\pi a}(\cos \theta _{1} - \cos \theta _{2}) \;\blacksquare\)
ดูวิธีทำ
จาก \(d\vec{B} = \frac{\mu _{0}}{4\pi}\frac{Id\vec{s}\times r̂}{r^{2}}\)
îĵk̂
\(d\vec{B} =\frac{\mu _{0}I}{4\pi (acosec\theta )^{2}}\)
\(dx00\)
\(\cos \theta \sin \theta 0\)
k̂
\(d\vec{B} =\frac{\mu _{0}Isin\theta dx}{4\pi (acosec\theta )^{2}}\)
k̂
\(\vec{B} =\frac{\mu _{0}I}{4\pi a^{2}}\int \sin ^{3}\theta dx\)
จาก \(cotθ = \frac{-x}{a}\)
\(x = -acot\theta\)
\(\frac{dx}{d\theta}= cosec^{2}\theta\)
\(\therefore dx = cosec^{2}\theta d\theta\)
\(^{\theta _{2}}k̂\)
จะได้ \(\vec{B} = \frac{\mu _{0}I}{4\pi a^{2}}\int \sin ^{3}\theta (acosec^{2}\theta d\theta )\)
\(_{\theta _{1}}\)
\(^{\theta _{2}}k̂\)
\(\vec{B} =\frac{\mu _{0}I}{4\pi a}\int \sin \theta d\theta\)
\(_{\theta _{1}}\)
\(_{\theta _{2}}\)
k̂
\(\vec{B} =\frac{\mu _{0}I}{4\pi a}(-\cos \theta )\)
\(_{\theta _{1}}\)
k̂
\(\vec{B} =\frac{\mu _{0}I}{4\pi a}(\cos \theta _{1} - \cos \theta _{2}) \;\blacksquare\)
พิจารณากรณีเส้นลวดยาวมากๆ
จะได้ \(θ_{1} \to 0\) และ \(θ_{2} \to π\)
k̂
\(\therefore \vec{B} =\frac{\mu _{0}I}{4\pi a}(\cos 0 - \cos \pi )\)
k̂
\(\vec{B} =\frac{\mu _{0}I}{2\pi a}\)