A 10-turn coil of wire having a diameter of 1.0 cm and a resistance of 0.30 Ω is in a 1.0 mT magnetic field, with the coil oriented for maximum flux. The coil is connected to an uncharged 3.0 μF capacitor rather than to a current meter. The coil is quickly pulled out of the magnetic field.


Afterward, what is the voltage across the capacitor?

Respuesta :

Answer:

The voltage across the capacitor = 0.8723 V

Explanation:

From the question, it is said that the coil is quickly pulled out of the magnetic field. Therefore , the final magnetic flux linked to the coil is zero.

The change in magnetic flux linked to this coil is:

[tex]\delta \phi = \phi _f - \phi _i[/tex]

    = 0 - BA cos 0°

[tex]\delta \phi =-BA \\ \\ \delta \phi =-B( \pi r^2) \\ \\ \delta \phi =(1.0 \ mT)[ \pi ( \frac{d}{2} )^2][/tex]

[tex]\delta \phi =(1.0 \ mT)[ \pi ( \frac{0.01}{2} )^2][/tex]

[tex]\delta \phi = -7.85*10^8 \ Wb[/tex]

Using Faraday's Law; the induced emf on N turns of coil is;

[tex]\epsilon = N |\frac{ \delta \phi}{\delta t} |[/tex]

Also; the induced current I = [tex]\frac{ \epsilon}{R}[/tex]

[tex]\frac{ \delta q}{ \delta t} = \frac{1}{R} (N|\frac{\delta \phi}{\delta t } |)[/tex]

[tex]\delta q = \frac{1}{R} N|\delta \phi |[/tex]

[tex]\delta q = \frac{1}{0.30} (10)| -7.85*10^8 \ Wb |[/tex]

[tex]\delta q = 2.617*10^{-6} \ C[/tex]

The voltage across the capacitor can now be determined as:

[tex]\delta \ V =\frac{ \delta q}{C}[/tex]

= [tex]\frac{ 2.617*10^{-6} \ C}{3.0 \ *10^{-6} F}[/tex]

= 0.8723 V