Gauss's Law for Magnetic Fields Flashcards
How do you determine the direction of a magnetic field due to a current in a wire?
- using the right hand rule
- thumb point in the direction of conventional current
- fingers curl in the direction of the magnetic field
Describe the Magnetic Field in a Solenoid
- magnetic field lines are always in a loop
- a solenoid appears to have a north pole at one end and a south pole at the other
- but actually the loops are continuous throughout
Solenoids and Divergence
- the divergence of the field of a solenoid is zero everywhere
- in any small volume dV, any field line going in is also going out as the lines are in loops so divergence is zero
Magnetic Dipole
- very similar field pattern to an electric dipole
- but the field lines are in loops whereas electric field lines stop and start on charges
- at the centre the magnetic field lines are in the opposite direction to the electric field lines
Gauss’s Law for Magnetic Fields - Differential Form
Equation
∇ . |B = 0
Gauss’s Law for Magnetic Fields - Integral Form
Description
- the total magnetic flux passing through any closed surface is zero, i.e for every field line entering the volume enclosed by the surface there is also a field line leaving it
- there are no point in space from which a magnetic field line diverges from or converges to
- magnetic monopoles do not exist
Gauss’s Law for Magnetic Fields
Derivation
∇ . |B = ΔV->0 lim 1/ΔV ∮|B.n^dA = ϕB
-net flux, ϕB, is telling you whether inside the closed surface you have a net source or a net sink of magnetic field lines and whether the net flow is in or out
-since there are no monopoles the net flux across any closed surface is always zero so divergence must also be zero:
∮|B.n^dA = 0
What is a vector field with zero divergence called?
- solenoidal fields
- all magnetic fields are solenoidal
- any vector field can be written as the sum of an irrotational field and a solenoidal field
Biot-Savart Law
Magnetic Field of a Moving Point Charge
|B(|r) = μ0/4π * q|v x |r /r²
Biot-Savart Law
Magnetic Field of a Steady Current
|B(|r) = I*μ0/4π * ∫ {d|I’ x |r / r²}
|I' = an element of length along the wire |r = the vector from the source to the point P
Biot-Savart Law
Magnetic Field of an Infinite Wire
B = I*μ0/2πa
a = perpendicular distance from the wire
Lorentz Force
Magnetic Field
|Fmag = Q(|v x |B)
The force Fmag, on a charge Q moving with speed v through a magnetic field B
Lorentz Force
Magnetic and Electric Field
|F = Q{|E + (|v x |B)}
The force |F, on a charge Q moving with speed v through an electric field E and a magnetic field B
Gauss’s Law for Magnetic Field’s - Integral Form
Equation
∮|B.n^dA = 0
Difference Between Electric and Magnetic Fields
- direction of magnetic field is perpendicular to the magnetic force, direction of electric field is parallel or antiparallel to force
- for determining magnetic field, speed and direction of the test charge must be considered
- for magnetic field, the component of the magnetic force in the direction of displacement is always zero
- electrostatic fields are produced by electric charges whereas magnetostatic fields are produced by electric currents