Magnetism
Magnetism
- Magnetism is the study of magnets and their properties.
Magnet
- A magnet is a material that produces a magnetic field.
- Magnets have two poles: South (S) and North (N).
- Like poles repel each other; opposite poles attract.
How to Make a Magnet
Ferromagnet:
- Start with a ferromagnetic material (e.g., iron).
- Heat the material and tap it repeatedly while it cools.
- This aligns the magnetic domains within the material, creating a permanent magnet.
Electromagnet:
- Wrap a coil of wire around a ferromagnetic core (e.g., iron).
- Pass an electric current (I) through the wire.
- The current creates a magnetic field.
- The strength of the magnetic field can be increased by increasing the current or the number of turns in the coil.
- MRI (Magnetic Resonance Imaging) utilizes electromagnets.
Magnetic Field (B)
- A magnetic field is a region around a magnet or current-carrying wire where magnetic forces can be detected.
- It has both direction and strength.
- Symbol: \vec{B}
- Unit: Tesla (T). Sometimes Gauss (G) is used (1 T = 10,000 G).
Magnetic Field Lines
- Magnetic field lines are used to visualize the direction and strength of a magnetic field.
- They point from the north pole to the south pole outside the magnet.
- The closer the lines, the stronger the field.
Notation Symbols for 3D Direction
- \odot: Out of the plane
- \otimes: Into the plane
Magnetic Moment (m)
- Magnetic moment is a measure of the strength and direction of a magnet.
- It is a vector quantity.
- Unit: A \cdot m^2
B-Field Strength
- Calculating B-field strength can be complex, but simplifications are possible in certain cases.
- Uniform Field: A magnetic field with constant magnitude and direction.
- Uniform Magnetic Field: A region where the magnetic field is uniform.
Magnetic Field Calculation
Straight Current Wire (Ampere’s Law):
- Magnitude: B = \frac{{\mu_0 I}}{{2 \pi r}}
- Direction: Determined by the right-hand rule (thumb in the direction of current, fingers curl in the direction of the magnetic field).
- \mu_0 = 4 \pi \times 10^{-7} T \cdot m/A (permeability of free space).
Center of a Current Loop:
- Magnitude: B = \frac{{\mu_0 I}}{{2r}}, where r is the radius of the loop.
- Direction: Perpendicular to the loop, determined by the right-hand rule.
Inside of a Solenoid:
- Magnitude: B = \mu_0 n I, where n is the number of loops per unit length of the solenoid (n = N/L, with N being the number of loops and L the length).
- Direction: Along the axis of the solenoid, determined by the right-hand rule.
Examples
Direction of Magnetic Field Around a Wire:
- The magnetic field lines wrap around the current in a counterclockwise fashion (based on the right-hand rule).
Current in a Wire Pointing into the Page:
- The magnetic field direction is Left.
Current in a Wire Pointing to the Right:
- The magnetic field above the wire is out of the page.
Current Carrying Loop (Magnetic Dipole Moment):
- The magnetic field at the center of the loop points along the direction of the magnetic dipole moment.
Current Carrying Loop as a Magnetic Dipole:
- Magnetic field lines leave a north pole and enter a south pole.
- The direction of the current determines which pole faces towards you.
Current Carrying Loop in an External Magnetic Field:
- A current carrying loop placed in an external magnetic field will experience a torque.
- The loop will rotate to align its magnetic dipole moment with the external magnetic field.
Example: Comparing Magnetic Field Magnitudes
- To determine which case has a larger magnetic field magnitude (at the center point), you need to compare the arrangements and distances.
Example: Find Magnetic Field at Specific Points
Given a current I in a wire, calculate the magnetic field at points A, B, and C using the formulas discussed earlier.
Solution:
- A: B = \frac{\mu_0 I}{2 \pi (2)} \uparrow
- B: B = \frac{\mu_0 I}{2 \pi (4)} \uparrow
- C:
- The distance from the wire to point C is \sqrt{2^2 + 4^2} = \sqrt{20} = 2\sqrt{5} meters.
- \tan(\theta) = \frac{4}{2}, so \theta = \tan^{-1}(\frac{1}{2}) = 63.43 degrees.
- The direction is such that the direction of the magnetic field at point C makes 63 degrees versus the x axis.
- Bx = \frac{\mu0 I}{2 \pi (2*\sqrt{5})} \cos(90-63)
- By = \frac{\mu0 I}{2 \pi (2*\sqrt{5})} \sin(90-63)