Новое решение
en/11.6.1.md
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| + | ### Statement | ||
| + | |||
| + | $11.6.1.$ [Insert the problem statement] | ||
| + | |||
| + | ### Solution | ||
| + | |||
| + | In the GHS, the EMP law for a vortex electric field is written: | ||
| + | |||
| + | $$C_E = - \frac{1}{c} \frac{d \Phi_B}{dt}$$ | ||
| + | |||
| + | The right screw, unlike the left screw, means a change of sign before the coefficient, so in the GHS the law for the vortex magnetic field looks like: | ||
| + | |||
| + | $$C_B = \frac{1}{c} \frac{d \Phi_D}{dt}$$ | ||
| + | |||
| + | In GHS, we have a displacement flow equal to the field flow. To convert to SI, we will use the standard ratios: | ||
| + | |||
| + | $$B_{GHS} = B_{SI} \cdot\sqrt{\frac{4\pi}{\mu_0}}$$ | ||
| + | |||
| + | $${\Phi_E}_{GHS} ={\Phi_E}_{SI} \cdot\sqrt{4\pi\varepsilon_0}$$ | ||
| + | After substituting this into the GHS equation and replacing the electric field flux with $\frac{\Phi_D}{\varepsilon_0}$: | ||
| + | |||
| + | $$C_B = \mu_0 \frac{d \Phi_D}{dt}$$ | ||
| + | |||
| + | Savchenko apparently made a typo in his answer to SI and wrote a connection with the flow of the electric field and not with the displacement flow. | ||
| + | |||
| + | #### Answer | ||
| + | |||
| + | [Insert a concise answer or boxed result] | ||
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| ### Statement | |||
| $11.6.1.$ [Insert the problem statement] | |||
| ### Solution | |||
| In the GHS, the EMP law for a vortex electric field is written: | |||
| $$C_E = - \frac{1}{c} \frac{d \Phi_B}{dt}$$ | |||
| The right screw, unlike the left screw, means a change of sign before the coefficient, so in the GHS the law for the vortex magnetic field looks like: | |||
| $$C_B = \frac{1}{c} \frac{d \Phi_D}{dt}$$ | |||
| In GHS, we have a displacement flow equal to the field flow. To convert to SI, we will use the standard ratios: | |||
| $$B_{GHS} = B_{SI} \cdot\sqrt{\frac{4\pi}{\mu_0}}$$ | |||
| $${\Phi_E}_{GHS} ={\Phi_E}_{SI} \cdot\sqrt{4\pi\varepsilon_0}$$ | |||
| After substituting this into the GHS equation and replacing the electric field flux with $\frac{\Phi_D}{\varepsilon_0}$: | |||
| $$C_B = \mu_0 \frac{d \Phi_D}{dt}$$ | |||
| Savchenko apparently made a typo in his answer to SI and wrote a connection with the flow of the electric field and not with the displacement flow. | |||
| #### Answer | |||
| [Insert a concise answer or boxed result] | |||