1. | \({\Large\frac{\mu_0i}{4R}}\) |
2. | \({\Large\frac{\mu_0i}{4R}}+{\Large\frac{\mu_0i}{2\pi R}}\) |
3. | \({\Large\Big(\frac{\mu_0i}{4R}+\frac{\mu_0i}{4\pi R}\Big)} \) |
4. | \({\Large\Big[\Big(\frac{\mu_0i}{4R}\Big)^2+\Big(\frac{\mu_0i}{2\pi R}\Big)^2\Big]^{1/2}} \) |
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1. | \(\dfrac{K}{a}\) | 2. | \(\dfrac{K}{b}\) |
3. | \(\dfrac{K}{a-b}\) | 4. | \(\dfrac{K}{a+b}\) |
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1. | \(\dfrac{\mu_0i}{4r}\) |
2. | \(\dfrac{\mu_0i}{4r}+\dfrac{\mu_0i}{2\pi r}\) |
3. | \(\dfrac{\mu_0i}{4r}+\dfrac{\mu_0i}{4\pi r}\) |
4. | \(\left[\left(\dfrac{\mu_0i}{4r}\right)^2+\left(\dfrac{\mu_0i}{4\pi r}\right)^2\right]^{\frac12} \) |
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1. | \(\dfrac{\mu_0~L~r~i}{V}\) | 2. | \(\dfrac{\mu_0~L~r~i}{2\pi~V}\) |
3. | \(\dfrac{\mu_0~L~r~i}{2V}\) | 4. | \(\dfrac{\mu_0~L~r~i}{4\pi~V}\) |
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1. | \(N\) | 2. | \(\dfrac 1N\) |
3. | \(2N\) | 4. | \(\dfrac{1}{2N}\) |
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1. | \(\lambda Br\) | 2. | \(\dfrac{\lambda Br}{r}\) |
3. | \(\dfrac{\lambda}{Br}\) | 4. | \(\dfrac{\lambda}{B^2r^2}\) |
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1. | \(\dfrac{q^2\phi}{2m}\) | 2. | \(\dfrac{q^2\phi}{2\pi m}\) |
3. | \(\dfrac{q^2\phi}{m}\) | 4. | \(\dfrac{q^2\phi}{\pi m}\) |
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1. | \(\dfrac{5}{\sqrt3r}\) | 2. | \(\dfrac{5}{\sqrt3\pi r}\) |
3. | \(\dfrac{5}{r}\) | 4. | \(\dfrac{5}{\pi r}\) |
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1. | \(25~\Omega\) in series | a resistance of
2. | \(\dfrac1{25}~\Omega\) in series | a resistance of
3. | \(25~\Omega\) in parallel | a resistance of
4. | \(\dfrac1{25}~\Omega\) in parallel | a resistance of
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