🧲Permanent Bar Magnet Active: Magnetic flux lines emerge from
North (Red) and loop into South (Blue).
B-Field: 35.4 G
📋 Observation Data Logger
#
Source
Loops (N)
Current I (A)
Core (μᵣ)
Probe Distance (cm)
Field B (G)
Angle θ (°)
🔢 Problem Solver Step-by-Step Derivation
Solved Answer
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💡 Magnets & Electromagnets Help Guide
What is Magnetism & Electromagnetism?
A permanent bar magnet creates a static magnetic
field due to aligned microscopic atomic electron spins within
ferromagnetic domains. Field lines emerge from the
North (N) pole and enter the
South (S) pole.
An electromagnet creates a magnetic field when
electric current flows through coiled wire loops (solenoid), as
discovered by Hans Christian Oersted in 1820. Unlike permanent
magnets, electromagnets can be turned on/off, have adjustable
strength, and can flip polarity instantly by reversing current.
🌟 Core Learning Goals:
Understand how magnetic field vectors point away from North
poles and toward South poles.
Observe how number of loops (N) and current (I)
linearly scale the solenoid magnetic field (B ∝
N·I).
Witness the dramatic 50× amplification achieved by inserting a
ferromagnetic Soft Iron Core (μᵣ = 50).
Use a compass to discover Right-Hand Grip Rule and track
alternating AC magnetic oscillations.
Key Scientific Formulas
1. Magnetic Field of a Solenoid (Ampere's Law): B = μ₀ · μᵣ · n · I = μ₀ · μᵣ · (N /
L) · I
Where μ₀ = 4π × 10⁻⁷ T·m/A, μᵣ is relative permeability,
n = N/L is turns per meter.
2. Magnetic Dipole Field on Axial Line (Bar Magnet): Baxis = (μ₀ / 4π) · (2M /
r³)
Where M is the magnetic dipole moment and r is the
distance from center.
3. Magnetic Dipole Field on Equatorial Line: Beq = (μ₀ / 4π) · (M / r³)
4. Lorentz Force on Moving Charged Particle: F = q · v · B · sin(θ)
5. Magnetic Flux through Surface:
Φ = B · A · cos(θ) (in Weber, Wb)
Interactive Laboratory Controls
Drag Objects: Click and drag the Bar Magnet /
Electromagnet, the Compass, or the Field Meter anywhere in the
play area.
Source Mode: Toggle between Permanent Bar
Magnet, DC Battery Electromagnet, and AC Alternator
Electromagnet in the left panel.
Flip Polarity: Click 🔄 Flip Polarity to
reverse poles or invert the DC voltage sign.
Bottom Toggles: Show or hide the Field Vector
Arrows, Compass needle, Digital Field Meter, and Earth
Geographic/Magnetic overlay.
Key Physics Experiments
Inverse Cube Law (Dipole B ∝ 1/r³): Drag the
Field Meter along the magnet axis at distances 10 cm, 20 cm, and
30 cm. Notice field drops by (1/2)³ = 1/8 and (1/3)³ = 1/27!
Testing Turns Dependency (B ∝ N): Switch to DC
Electromagnet. Keep voltage fixed at 5 V and increment loops
from 1 to 4. Observe exact proportional scaling of B.
Soft Iron Core Amplification: Compare the field
of an Air Core (μᵣ = 1.0) with a Soft Iron Core (μᵣ = 50.0).
Record rows in the Data Logger to calculate amplification
factor.
AC Magnetic Reversal: Switch to AC
Electromagnet, set frequency to 0.5 Hz, and watch the compass
needle swing smoothly back and forth as the magnetic field
oscillates.
Frequently Asked Questions
Q: Why does the compass North pole point towards Earth's
North?
Earth behaves like a giant bar magnet whose
magnetic South pole is geographically near the North
Pole. Opposites attract, so the North pole of the compass needle
points to geographic North.
Q: What is the unit relationship between Gauss and
Tesla?
1 Tesla (T) = 10,000 Gauss (G). Therefore, 1 Gauss = 100
microTesla (μT) = 10⁻⁴ T.
Q: Why do magnetic field lines never cross?
At any point in space, the net magnetic field has only one
resultant vector direction. If two lines crossed, a compass needle
at the intersection would have to point in two directions at once,
which is physically impossible.
🎉
Challenge Complete!
Great job! You achieved the target magnetic parameters.