| Command, Control, and Monitoring Technologies | Research
and Technology 2002
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| Solenoid Inter-Force (SIF) Calculator |
| The Lorentz force is the well-known force exerted on a charged particle of charge q and velocity v in a magnetic field B: | The final force formula given in figure 2 is found by combining Equations (3) and (4). This is the force that pushes coil 2 above coil 1 while balancing gravity. The levitation height h is dependent on the product of the currents in both coils (I1 and I2) as well as the mass of coil 2. Note that if the currents I1 and I2 flow in the same direction, the force is attractive. In order to levitate, the currents must be in opposite directions.
Contacts: Dr. R.C. Youngquist (Robert.Youngquist1@ksc.nasa.gov),
YA-C3-E, (321) 867-1829; and Dr. J.C. Simpson, YA-D7, (321) 867-6937 |
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When a charged particle, such as an electron or proton with a linear
velocity, encounters a magnetic field, the Lorentz force results in a spiral
trajectory, where the circular portion of the path is perpendicular to
the B field. |
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| Equation (2) is useful in describing a solenoid coil configuration. This
is the case in figure 1, where the bottom coil (coil 1) is stationary and
has a steady-state current of I1. The upper coil (coil 2) in figure 1,
which has a steady-state current I2, slides along a vertical rod, maintaining
axial symmetry. A form of the force equation that lends itself to evaluation by computer is: |
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where I2 is the current and A2 is the cross-sectional area
of coil 2 wire, ak is the radius of the kth wire loop of coil 2, and Bk
is the field at the position of the kth wire loop of coil 2. The position
of the kth wire loop is specified by and z = zk.Now sum the simple analytic expressions for the magnetic field of a circular current loop over all loops of the solenoid (see “Solenoid Inductance and B-Field Calculator,” KSC Research and Technology 2000-2001 Report): |
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The final force formula given in figure 2 is found by combining Equations (3) and (4). This is the force that pushes coil 2 above coil 1 while balancing gravity. The levitation height h is dependent on the product of the currents in both coils (I1 and I2) as well as the mass of coil 2. Note that if the currents I1 and I2 flow in the same direction, the force is attractive. In order to levitate, the currents must be in opposite directions.
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Figure 1. Lorentz Levitation Test
Figure 2. SIF Analytic Formulas |
Figure 3. Measured Versus Calculated Data
Figure 4. SIF Windows Panel |
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