Calculating the terminal velocity of a magnet falling through a copper coil

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SUMMARY

This discussion focuses on calculating the terminal velocity of a magnet falling through a copper coil using specific parameters and equations. The magnet dimensions are defined as d = 0.0127 m and r = 0.00238 m, with a mass of 0.0017 kg. The code provided calculates the terminal velocity to be 1E-4 m/s, assuming sufficient turns in the coil to simulate a copper tube. The results indicate that the experimental terminal velocity is expected to be higher than the calculated value due to the less effective damping of copper coils compared to solid copper tubes.

PREREQUISITES
  • Understanding of terminal velocity calculations in physics
  • Familiarity with electromagnetic principles, particularly eddy currents
  • Knowledge of material properties, specifically copper resistivity and permeability
  • Proficiency in MATLAB or similar programming for numerical integration
NEXT STEPS
  • Explore the effects of varying magnet strength on terminal velocity
  • Investigate the impact of different wire sizes on eddy current formation
  • Learn about the principles of electromagnetic damping in coils
  • Conduct a cost analysis for the proposed magnet and coil system
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Physicists, electrical engineers, and anyone involved in experimental design related to electromagnetic systems and damping mechanisms.

rayjbryant
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The magnet being used

[CODE lang="matlab" title="The main body code."]% magnet dimensions [m]

d = .0127;
r = .00238;

%mass of magnet [kg]

m_w = .0017;

% other constants

u_0 = 1.26E-6; % permeability of free space constant T m/A
g = 9.81; % gravitational constant in/s^2

%coil properties [22 gauge wire] [m]

a = .00635; %radius
w = .000635; %width of wire
N = 100; % number of turns
c = pi*a*2; %circumference
wl = c*N; %wire length
cs = pi*(w/2)^2; %cross sectional area
rho = 1.7e-8; % resistivity of copper [ohm/m]
wr = (rho*wl)/cs; % resistance in wire [ohm]
lt = 0.3048; % length of tube

%magnetic properties

sm = 72730000; % magnetic surface charge density [Mx/m^2]

qm = pi*sm*r^2; %

eff_dist = .003175;

%terminal velocity

p = qm*d;

x = d/a;

val = scalingfunction(x);

v = (8*pi*m_w*g*rho*a^2)/(u_0^2*qm^2*w*val);
[/CODE]

[CODE lang="matlab" title="The scaling function code."]function [val] = scalingfunction(x)
fun = @(x,y) ((1./(y.^2+1).^(3/2))-(1./((y+x).^2 + 1)).^(3/2)).^2;
val = integral(@(y) fun(x,y),-Inf,Inf);
end[/CODE]

terminal velocity ends up being: 1E-4 m/s
 

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rayjbryant said:
I'm attempting to calculate the terminal velocity of a magnet falling through a copper coil by assuming there are enough turns to treat it as a copper tube.
How is your coil terminated? Are the ends connected together? How are eddy currents going to form in a coil to generate a retarding force?

When you use a copper tube in your simulation, do you get the expected result?
 
Yes, the ends are connected to allow current to flow and eddy currents to form. The desired effect was achieved with a physical model using a weaker magnet and 20 gauge coil but not enough damping or current flow occurred. The purpose of this code is to find a combination of magnet strength, wire size, and turn number to build a model that will work to desired specifications. After which a cost analysis will be performed to see if the system is economically feasible to use in the desired commercial application.
 
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And sorry I misread the first part of your post. The equation used in the code to calculate the terminal velocity automatically assumes the apparatus is a solid tube. I've performed several copper tube and magnet experiments as well as observed quite a few, and none have a terminal velocity as low as 1E-4 m/s. If any error does occur, it should be an experimental terminal velocity higher than the computer model, since copper coils are not as effective at damping as copper tubes.
 
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