Question #56229

A long solenoid of radius 2 cm has 100 turns/cm and carries a current of 5A. A coil of radius 1 cm having 100 turns and a total resistance of 20 Ω is placed inside the solenoid coaxially. The coil is connected to a galvanometer. If the current in the solenoid is reversed in direction, find the charge flown through the galvanometer and how?
1

Expert's answer

2015-11-10T03:06:26-0500

Answer on Question #56229, Physics / Electromagnetism

A long solenoid of radius 2cm2\mathrm{cm} has 100 turns/cm and carries a current of 5A. A coil of radius 1 cm having 100 turns and a total resistance of 20Ω20\Omega is placed inside the solenoid coaxially. The coil is connected to a galvanometer. If the current in the solenoid is reversed in direction, find the charge flown through the galvanometer and how?

Solution.

I=5AI = 5\mathrm{A} –is current through solenoid; rs=2cm=0.02mr_s = 2\mathrm{cm} = 0.02\mathrm{m} – radius of solenoid;

rc=1cm=0.01mr_c = 1\mathrm{cm} = 0.01\mathrm{m} – radius of the coil; N=100N = 100 – number of coil turns;

R=20ΩR = 20\Omega – is the total resistance of coil; n=100turnscm=104turnsmn = 100\frac{\mathrm{turns}}{\mathrm{cm}} = 10^4\frac{\mathrm{turns}}{\mathrm{m}};

α=0\alpha = 0 – the angle between axes of coil and solenoid.


q=t1t2Idt=t1t2EindRdt=1Rt1t2Einddt| q | = \left| \int_ {t 1} ^ {t 2} I d t \right| = \left| \int_ {t 1} ^ {t 2} \frac {\mathrm {E} _ {i n d}}{R} d t \right| = \left| \frac {1}{R} \int_ {t 1} ^ {t 2} \mathrm {E} _ {i n d} d t \right|

Eind=dΦdtE_{ind} = -\frac{d\Phi}{dt} – is electromotive force of the induction; t1,t2t1, t2 – moments of time before and after change current direction;


q=1Rt1t2dΦdtdt=1RΦ(t2)Φ(t1)| q | = \left| \frac {1}{R} \int_ {t 1} ^ {t 2} \frac {d \Phi}{d t} d t \right| = \frac {1}{R} | \Phi (t 2) - \Phi (t 1) |

Φ=NBScosα\Phi = NBS\cos \alpha – the total magnetic flux trough coil; S=πrc2S = \pi r_c^2 – area of the coil;


q=NScosαRB(t2)B(t1)| q | = \frac {N S \cos \alpha}{R} | B (t 2) - B (t 1) |


Let B0B_0 – magnetic field before current reversed, then B(t2)=B0B(t2) = -B_0, B(t1)=B0B(t1) = B_0

q=NScosαRB0B0=2B0NScosαR| q | = \frac {N S \cos \alpha}{R} | - B _ {0} - B _ {0} | = \frac {2 B _ {0} N S \cos \alpha}{R}

B0=μ0InB_{0} = \mu_{0}In – magnetic field in solenoid;

μ0=4π107H/m\mu_0 = 4\pi *10^7\mathrm{H / m} – magnetic constant;


q=2μ0nNSIRcosα=2πμ0nNrc2IRcosα| q | = 2 \mu_ {0} n N S \frac {I}{R} \cos \alpha = 2 \pi \mu_ {0} n N r _ {c} ^ {2} \frac {I}{R} \cos \alphaq=23.1443.14104102(102)2520cos01.97104(C)| q | = 2 * 3. 1 4 * 4 * 3. 1 4 * 1 0 ^ {4} * 1 0 ^ {2} * (1 0 ^ {- 2}) ^ {2} * \frac {5}{2 0} * \cos 0 \approx 1. 9 7 * 1 0 ^ {- 4} (\mathrm {C})


According to Lenz's law, direction of current in coil is the same as direction of current in solenoid before direction reversed.

Answer: 1.97104C1.97 * 10^{-4} \, \text{C}, direction of current in coil is the same as direction of current in solenoid before direction reversed.

http://www.AssignmentExpert.com/


Need a fast expert's response?

Submit order

and get a quick answer at the best price

for any assignment or question with DETAILED EXPLANATIONS!

Comments

No comments. Be the first!
LATEST TUTORIALS
APPROVED BY CLIENTS