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F' Isica Electromagn Etica: Tarea #1: @ccmejia

The document contains 5 physics problems related to electromagnetism: 1) Calculating the equivalent capacitance of a capacitor circuit and the total charge. 2) Finding the current in a circuit with batteries, resistors, and voltages given. 3) Using Ampere's law to find the magnetic field of a hollow conducting cylinder. 4) Finding the induced electromotive force in a semi-circular conducting loop in a changing magnetic field. 5) Deriving the resistance of a hollow cylindrical conductor with current flowing radially through its walls.

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Majo Jaimes
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0% found this document useful (0 votes)
45 views3 pages

F' Isica Electromagn Etica: Tarea #1: @ccmejia

The document contains 5 physics problems related to electromagnetism: 1) Calculating the equivalent capacitance of a capacitor circuit and the total charge. 2) Finding the current in a circuit with batteries, resistors, and voltages given. 3) Using Ampere's law to find the magnetic field of a hollow conducting cylinder. 4) Finding the induced electromotive force in a semi-circular conducting loop in a changing magnetic field. 5) Deriving the resistance of a hollow cylindrical conductor with current flowing radially through its walls.

Uploaded by

Majo Jaimes
Copyright
© © All Rights Reserved
We take content rights seriously. If you suspect this is your content, claim it here.
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Download as PDF, TXT or read online on Scribd
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FÌsica Electromagnética: Tarea #1

@ccmejia

1
However, note that the shifting charge can move to the to th
bottom plates of both capacitor 1 and capacitor 2. capac
Because there is more than one route for the shifting equiv
@ccmejia FÌsica Electromagnética: Tarea #1 Problema 1

Problema 1
Encuentre la capacitancia equivalente para We first reduce
la combinación the The equivalent
de condensadores mostrada enofla Fig.The equivalent
1. Calcule la of
carga total almacenada en el condensador C circuit to a single
teniendo en cuenta que parallel capacitors
la diferencia de potencial series capacitors
que alimenta
N
1
el circuito es de 12.5 voltios. capacitor. is larger. is smaller. b
d
A A

C1 = C2 = C 12 =
12.0 µF 5.30 µF 17.3 µF
V V B V C 123 = 12.5
B 3.57 µF
C3 = C3 =
4.50 µF 4.50 µF

(a) (b) (c )
Figura 1
Parallel capacito
Series capacitors and
Applying V = q/C yields their equivalent h
their equivalent have
Problema 2 the same q (“seri-q”).
the potential difference. the same V (“pa
Las fems y las resistencias dispuestas en el circuitoq 12 ilustrado
= por la Fig. 2 tienen
q 12 = los siguientes valores:
E1 = 4,4V , E1 = 2,1V , r1 = 2,3Ω, r2 = 1,8Ω y R = µC
44.6 44.6iµC
5,5Ω. ¿Cuál es la corriente que recorre el circuito?
C1 = V1 =
¿Cuál es la diferencia de potencial entre los puntosCa12y=b? C 12 = V 12 =
17.3 µF 12.0 µF 2.58 V 5
17.3 µF 2.58 V
12.5 V a
q3 = 12.5 V q3 = q3 =
44.6i µC 44.6 µC 12.5 V 44.6 µC
1 C3 = 2 C3 = V3 = C3 =
Battery 1 4.50 µF Battery 2 4.50 µF 9.92 V 4.50 µF 9
r1 i r2

b( f ) R c (g) (h)

Fig. 225-10
Figura (a) – (d) Three capacitors are reduced to one equiva
Working backwards to get the charges.

Problema 3
El cilindro hueco conductor de la Fig. 3, de radios R1 y R2 , conduce una corriente I uniformemente distribuida
en su sección transversal. Usando la ley de Ampere probar que el campo magnético a distancias r > R2 es
µ0 I(r 2 −R12 )
B = µ0 I/2πr, que el campo magnético para R1 < r < R2 es B = 2π(R 2 −R2 )r y que es B = 0 para r < R1 .
2 1

Problema 4
La Fig. 4 muestra un circuito conductor que consiste en una semi circunferencia de radio r = 0,2m y
tres secciones rectas. La semi circunferencia está dispuesta en una región dónde hay un campo magnético
perpendicular al área encerrada por la semi circunferencia; el campo magnético viene dado por B = 4,0t2 +
2,0t + 3,0, siendo las unidades de B el tesla y las unidades de t los segundos. Cuál es la magnitud y la
dirección de la fem inducida en el circuito por el campo B para t = 10s.

2
@ccmejia FÌsica Electromagnética: Tarea #1 Problema 5

Figura 3

r/ 2
– +
bat

Figura 4

Problema 5
Un conductor cilı́ndrico hueco, de longitud L, tiene radios R1 y R2 . Se aplica una diferencia de potencial
entre las superficies interior y exterior de modo que la corriente I fluya en dirección radial hacia afuera.
Demostrar que si σ es la conductividad del material, la resistencia es R = ln (R2 /R1 )/2πσL.

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