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23 Mar 2013

Force of a Magnetic Field on a Current-Carrying Wire


Force of a Magnetic Field on a Current-Carrying Wire



     A current-carrying wire in a magnetic field experiences a force. The magnitude and direction of this force depend on four variables: the magnitude and direction of the current (I), the length of the wire (L), the strength and direction of the magnetic field (B), and the angle between the field and the wire (Θ). The force can be described mathematically by the vector cross-product:

     F = I L X B      

Or in scalar terms:

     F = I L B SinΘ

     When current is in amperes, length in meters, and magnetic field in teslas, the force
is in newtons.
     The direction of the force is perpendicular to both the current and the magnetic field, and is predicted by the right-hand cross-product rule.
     For a more detailed discussion of the above material, read the following pages in your textbook (for Physics 212, pages 736 to 738 and 750 to 751.)

Equipment

     O’Haus Four-Beam Balance
     Lab Stand (V-Shaped Base and Attached Rod )
     Pasco Current Balance (SF-8607), consisting of
1.      Main Unit
2.      Magnet Assembly, with Six Magnets
3.      Six Different Current Loop Boards*
     Kelvin 200LE Multimeter
     Pasco Low Voltage AC/DC Power Supply (SF-9584A)

*For each of the current loop boards, the length of the straight-line segment that will lie in the magnetic field is as follows:

Current Loop          Length

SF 40                       1.0 cm
SF 37                       2.0 cm    
SF 39                       3.0 cm
SF 38                       4.0 cm
SF 41                       6.0 cm
SF 42                       8.0 cm

(These lengths are the distances between the centers of the vertical wires bringing current into and out of the segment.)

Objective

     To verify the relation

     F = I L B     (for Θ = 90 degrees)

with two sets of measurements:
1.      Holding L and B constant, vary the current, and measure how the force on the wire varies with current.
2.      Holding I and B constant, vary the length, and measure how the force on the wire varies with length.

Procedure

  1. Preliminary Set-Up

     1.   Place the magnet assembly on the tray of the four-beam balance.
     2.  Mount the main unit of the current balance on the vertical rod supported by
      the lab stand.
3.   Plug current loop board SF 39 (3.0cm) into the main unit. Adjust its height           and position so that the straight wire segment is centered between the (white and red)
magnetic poles. Make sure the current loop board does not touch the magnetic poles.
4.  With the power supply off, attach two leads to the  +  and  -  terminals of the
DC (left) side of the power supply. Connect the  +  lead to the 10A terminal of the
multimeter. Connect the COM terminal of the multimeter to the top of the current
balance. Connect the  -  power supply lead to the other terminal of the current balance.
     5.  Set the multimeter on 20m/10A and on DC, and turn it on.
     6.  In the power supply, turn the voltage and current dials counterclockwise to the
zero position.

  1. Data Collection for Force versus Current

     1.Record the weight of the magnet (when no current is passing through the wire.)
     2.  Turn on the power supply, (V and I should both read zero.)
     3.  Turn the voltage dial about 1/4 turn clockwise.
     4.  Slowly  turn the current dial until the current is one amp. Notice that the a vertical
     force has changed the reading of the balance. Take a new balance reading. (The
     change in “weight” is the force that the magnetic field is exerting on the wire.)
  1.  Repeat step 4 for two, three, four, and five amps.

C.  Data Collection for Force versus Wire Length

      1.  Reduce the current to zero. Replace the current loop with the 1.0 cm current
       loop.
  1. With current at zero, record the weight.
  2. Raise the current to 5 amps and record the new current balance reading.
  3. Repeat steps 1 to 3 with each of the six current loops.

D. Magnetic Field Strength

      Use the Gaussmeter on the instructor’s desk to measure the magnetic field
of your magnet assembly.

Computations

  1. Variation of Force with Current

  1. For each current setting, find the force, which is the difference between
the magnet assembly weight and the balance reading. Convert grams to kilo-
grams and multiply by  g   to obtain the force in newtons.
  1. Calculate the theoretical value of the force for each current setting using

F = I L B

  1. Compare each measured force with the corresponding theoretical value
and calculate each percent difference.
  1. Plot the measured force versus current and obtain a best-fit straight line.  
Compare the value of its slope with the product of L and B.

  1. Variation of Force with Length

  1. Using the force versus length data repeat steps 1 to 3 of the previous computations.
  2. Plot measured force versus length and obtain a best-fit straight line. Compare
its slope with the product of I and B.