Exam Solutions for PHY2049, Spring 2005 - Electromagnetism, Exams of Calculus

The solutions to exam 2 for the physics 2049 - electromagnetism course at the university of x, given in spring 2005. The solutions cover various problems related to current flow, magnetic fields, and torque.

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PHY2049 Spring 2005
1
Prof. Darin Acosta
Prof. Paul Avery
March 9, 2005
PHY2049, Spring 2005
Exam 2 Solutions
1. Two identical light bulbs A and B are connected in series to a constant voltage source.
A wire is then connected across B. What is the brightness of A relative to its former
brightness?
A light bulb will have a certain resistance R. The light it emits will be proportional to the
energy dissipated by this resistance: 2
PiR=. So when two identical light bulbs are
connected in series to a constant voltage V, the current passing through the circuit is
/2iV R=and the power dissipated in light bulb A is:
22
12
44
VV
PR
R
R
==.
Now when a wire is connected across light bulb B, that means that the resistance is
bypassed by a wire in parallel to the bulb (i.e. the bulb is shorted out by a jumper). The
resistance of bulb B becomes zero, and the current in the circuit is /iVR
=
. This current
is twice as high as before, but the power dissipated by light bulb A will be four times
more:
2
21
4
V
PP
R
==
Answer: 4
2. In the circuit shown, what is the current (in amps) flowing through the 18V battery?
Let 1
i be the current through the 18V battery, 2
i the current through the middle branch
with the 6V battery, and 3
i the current through the rightmost branch.
By Kirchoff’s junction rule: 123
iii=+.
By Kirchoff’s voltage sum rule applied to the rightmost loop:
23
32
6V 12 24
0.5 0.25
ii
ii
+Ω=
⇒= +
pf3
pf4
pf5

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Prof. Darin Acosta Prof. Paul Avery March 9, 2005 PHY2049, Spring 2005

Exam 2 Solutions

  1. Two identical light bulbs A and B are connected in series to a constant voltage source. A wire is then connected across B. What is the brightness of A relative to its former brightness?

A light bulb will have a certain resistance R. The light it emits will be proportional to the energy dissipated by this resistance: P = i R^2_. So when two identical light bulbs are connected in series to a constant voltage V, the current passing through the circuit is i_ = V / 2 Rand the power dissipated in light bulb A is: 2 2 (^1 4 )

V V

P R

R R

Now when a wire is connected across light bulb B, that means that the resistance is bypassed by a wire in parallel to the bulb (i.e. the bulb is shorted out by a jumper). The resistance of bulb B becomes zero, and the current in the circuit is i = V / R. This current is twice as high as before, but the power dissipated by light bulb A will be four times more: 2 2 4 1

V

P P

R

Answer: 4

  1. In the circuit shown, what is the current (in amps) flowing through the 18V battery?

Let i 1 be the current through the 18V battery, i 2 the current through the middle branch

with the 6V battery, and i 3 the current through the rightmost branch.

By Kirchoff’s junction rule: i 1 (^) = i 2 (^) + i 3_._

By Kirchoff’s voltage sum rule applied to the rightmost loop:

2 3 3 2

6V 12 24

i i i i

By Kirchoff’s voltage sum rule applied to the leftmost loop:

1 2 2 3 2 2 2 2 2 2

2

3 2 1 2 3

18V 6 6V 12

i i i i i i i i i i

i

i i i i i

Answer: 1.0 Amps through 18V battery

  1. An electron is accelerated from rest by a potential difference of 8.0 kV. It then enters a uniform magnetic field of magnitude 1.0 T with its velocity perpendicular to the direction of the field. Calculate the radius in meters of its path in the magnetic field.

Setting the centripetal acceleration, a = v^2^ / r, equal to the acceleration due to the magnetic force, FB / m = qvB / m, yields the following relation for the radius of curvature

for a charged particle moving in a uniform magnetic field: mv r qB

To get the velocity, one must realize that the kinetic energy of the electron after accelerating from rest across an electric potential equals the initial potential energy:

( )( )(^ )

2

31 19 4 19

2 2 9.11 10^ kg^ 1.6^10 8000 V 3.0 10 m 1.6 10

E (^) K mv eV

mv meV

meV r qB

− − − −

× ×

⇒ = = = ×

×

Answer: 3.0 × 10 −^4 m

  1. A solenoid is 3.0 cm long and has a radius of 0.50 cm. It is wrapped with 500 turns of wire carrying a current of 2.0A. What is the magnetic field at the center of the solenoid?

One can apply Ampere’s Law to determine that for a very long solenoid, the magnetic field inside is given by:

B = μ 0 ni, where n is the number of windings per unit length and i is the current in the

wire. This formula will hold approximately for the center of a solenoid of finite length. Thus,

( ) (^ )

7 2 0

4 10 2 4.2 10 T

B = μ ni = π × −^ ^  = × −

Answer: 4.2 × 10 −^2 T

  1. A capacitor with an initial potential difference of 100V is discharged through a resistor when a switch between them is closed at t =0. At t =5 s, the potential difference across the capacitor is 50V. What is the time constant of the circuit?

A capacitor in series with a resistor satisfies the following differential equation by applying Kirchoff’s voltage sum rule:

0

dq q R dt C

The solution is: q t ( ) = q e 0 −^ t^ / RC

So the voltage on the capacitor is C ( ) 0^ t^ /^ RC^ 0 t^ / RC

q V t e V e C

= −^ = −

Plugging in for what we know:

0 5/ 0

0 100 V

5 50 V

ln 2

5 7.2 s ln 2

C RC C

RC

V V

V t V e

RC

τ RC

Answer: 7.2 s

  1. In the figure shown, two long straight wires with separation d carry currents i 1 and i 2 =2 i 1 out of the page. At what point on the x -axis shown is the net magnetic field due to the currents equal to zero?

The magnetic field from each wire will be in the same direction for x < 0 and x > d. Only for 0 < x < d are the fields lines opposite in direction. (Use the right-hand rule to get the direction). Thus, the net magnetic field is:

0 1 2

1 2 1 1

i i x d x i d x i x i d x i x d d x x

Answer: d /

  1. A horizontal power line carries a current of 7000A from south to north. Earth's magnetic field, with a magnitude of 60μT, is directed toward the north with a dip angle 60° downward relative to the horizontal. Find the magnitude of the magnetic force acting on a 100 m length of power line.

The magnetic field and the power line both point north, but the magnetic field points into the Earth at an angle of 60°.

The force on a current carrying wire is given by: F = i L × B

So the force points west with magnitude:

F = iLB sin θ = ( 7000 )( 100 )( 60 × 10 −^6 )( sin 60 )=36.4 N

Answer: 36.4 N

S N

i

B