Multiloop circuit, magnetic force on a current carrying wire, Ampere's Law

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SUMMARY

The discussion covers three key topics in electromagnetism: multiloop circuits, magnetic forces on current-carrying wires, and Ampere's Law. For the multiloop circuit with resistors R1 = 5.76 Ω and R2 = 18.7 Ω powered by a 13.8 V battery, the current i1 was incorrectly calculated as 1.59 A. The magnetic force on a wire of length 62.9 cm carrying a 0.480 A current in a magnetic field was analyzed, revealing that only the z-component of the force was significant. Lastly, using Ampere's Law, the relationship between the magnetic field around a long circular pipe and a parallel wire was explored, leading to a calculation error in determining the current needed in the wire to achieve a specific magnetic field ratio.

PREREQUISITES
  • Understanding of Ohm's Law and circuit analysis
  • Familiarity with magnetic fields and forces on current-carrying conductors
  • Knowledge of Ampere's Law and its applications
  • Ability to perform vector calculations in physics
NEXT STEPS
  • Study the principles of multiloop circuit analysis in detail
  • Learn about the calculation of magnetic forces on current-carrying wires
  • Explore advanced applications of Ampere's Law in electromagnetic theory
  • Investigate the effects of varying magnetic fields on current-carrying conductors
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Physics students, electrical engineers, and educators seeking to deepen their understanding of electromagnetism and circuit analysis.

irnubcake
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1. Multiloop circuit
In Fig. 27-71, R1 = 5.76 , R2 = 18.7 , and the ideal battery has emf = 13.8 V. (a) What is the size of current i1?

http://img253.imageshack.us/img253/9926/fig2771dw3.gif

Relevant equations
i = V/R

The attempt at a solution
I redrew the 3 resistors (R2s) as parallel resistors. So i1 would be in the middle. Then all the resistances would have the same voltage 13.8V. So
i1 = V/R2 = 13.8V/18.7 = 1.59 A. It's wrong though.

2. Magnetic Force on a Current-Carrying Wire
A wire 62.9 cm long carries a 0.480 A current in the positive direction of an x-axis through a magnetic field with an x component of zero, a y component of 0.000230 T, and a z component of 0.0120 T. Find the magnitudes of x, y, and z components of the force on the wire.

Relevant equations
Magnitude of the force on a current carrying wire = (current)*(length)*(magnetic field)*(sin (angle between the directions of field and the length))

The attempt at a solution
The length of wire is along the x axis, so the angle between the wire and the x-axis = 0. The angle between the x-axis and y-axis = 90 degrees, between x and z is also 90 degrees:
force magnitude of x component = 0
force magnitude of y component = 0.480A x 0.629m x 0.000230T x sin 90
force magnitude of z component = 0.480A x 0.629m x 0.0120T x sin 90

Only the first one's right.

3. Ampere's Law
In Fig. 29-63, a long circular pipe with outside radius R = 2.65 cm carries a (uniformly distributed) current i = 9.16 mA into the page. A wire runs parallel to the pipe at a distance of 3.00R from center to center. Find the magnitude of the current in the wire in milliamperes such that the ratio of the magnitude of the net magnetic field at point P to the magnitude of the net magnetic field at the center of the pipe is 3.93, but it has the opposite direction.

http://img442.imageshack.us/img442/8181/fig2963ho7.gif

Relevant equations
Magnetic field at distance r outside long straight wire with current =
(μ0 x i)/(2 x pi x r)
Magnetic field around Amperian loop = μ0 x current enclosed

The attempt at a solution
(Magnetic Field at pt P) / (Magnetic Field at the center of the pipe) = 3.93

so: (μ0 x i)/(2 x pi x R) = 3.93 x (μ0 x current enclosed)
...i = 3.93 x current enclosed x 2 x pi x R
= 3.93 x 9.16 mA x 2pi x 0.0265m = 0.00599 (mA)(m)
The units should only have mA so the answer is wrong.
 
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1. You are corrrect in assuming that the R2s are in parallel and that they will share the same voltage. The emf divides over this parallel combination and R1 though. What you can assume is that the three parallel branches will draw the same current, I1. This means that 3 x I1 will flow through R1. Use the eq.

Emf = V1 + V2

to solve for I1.

2. The components of the magnetic field and the length vector form a triad of vectors where the length vector points along the x-axis.

The direction of the force components are obtained by rotating the length vector towards each of the magnetic field components.

By rotating the length vector towards the y magnetic field component we obtain a force component in the negative z-axis direction. The z component of the force therefore involves the y component of the magnetic field.
 

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