All directions of the red arrows were pointing consistently as it was moved around the magnet
We can observe that at the poles the magnetic field lines point out and curve around in a circular pattern, a more accurate depiction
Our model of the Iron fillings experiment (left). The side surface and one that entirely surrounding both poles have a net flux of 0 because the number of field lines enter the circle equals the ones exiting.
Next we experimented how magnetic field affect moving charged particles in the oscilloscope
Making an magnetic field pointing into the screen (above) pointing outward of screen (below)
Prof Mason manipulating the electrons inside the poorly-shielded oscilloscope tube.
We then observe what happens to a non-magnetic copper wire near a magnet when we pass a current through the wire:
The current going through the wire is our velocity vector going horizontally and the magnetic field runs between the north and south poles is our magnetic field vector going vertically. Using the right-hand rule, we confirmed the direction the wire move due to Force.
Next, we experimented with a copper rod and applied some current through it to see which direction it rolls
Just as what the right-hand rule suggested, it rolled outwards
Current passing through the copper rod. We conclude Force is proportional to current as we turn it up
All of the measurements including the final equation we derived to calculate the strength of the magnetic field is shown above, and the answer we came up with was roughly .0.011T, which seems a little low but not too unreasonable.
We wrapped up the day with several more calculations of non-uniform magnetic field which torque is involved:

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