Hello it's a me again Drifter Programming! Today we continue with Electromagnetism to get into Exercises/Examples all around the Mutual and Self Induction "chapter" we covered in the previous articles. By that I mean examples around Mutual Inductance, Self Induction, Magnetic Energy Density, R-L circuits and L-C circuits. R-L-C circuits have been covered mostly theoretically and so no mathematical applications will be covered yet. So, without further do, let's get started!
To stay organized each article/topic will be covered on it's own...as always!
First up the Mutual Inductance and induced emf between two conductors (we covered coils on N turns that are more interesting).
Let's consider two insulated wires that are wound into a common cylinderical former of l=0.1m length. The cross-sectional area is A = 0.05m^2. The first wire has N1 = 100 turns, whilst the second one has N2 = 300 turns. Let's calculate:
- The Mutual inductance (M) of the two wires
- If a current I1 is flowing in the first wire and increases from 0 to 10A in 0.1s, what will be the emf generated on the second wire? Will the produced emf/current act in the same or opposite sense?
As we know from the corresponding article, Mutual inductance is a purely geometrical quantity which doesn't depend on the current and is given by:
For our example the Mutual inductance of the two wires is therefore:
The induced emf generated around the second loop can be calculated by:
The negative sign already shows us that the current on the second wire circulates in opposite sense. According to Lenz's law: "The induced emf/current always tries to oppose the change in magnetic flux that caused it!".
By entering the values of each quantity we can calculate the actual emf, which is:
If the resistance of the second wire was also given to us, then the induced current could be calculated using Ohm's law as:
Let's now consider two identical coils that are wound on a ring-shaped iron core with relative permeabilty μr = 500. Each coil has 100 turns and the cross-sectional area is A = 3cm^2. The magnetic path length is l = 20cm. Calculate the Mutual Inductance between the coils by calculating the inductance of each coil and then using:
This example contains Mutual Inductance and Self Induction!
The inductance of each coil is also a purely geometrical quantity. As we know from the article of the series this inductance is calculated as:
For the values of our example the inductance of each coil is therefore:
Using the given equation the Mutual inductance is:
Note: Being wound on the same iron core means that k = 1.
Continuing on with Self Inductance...
Let's consider a solenoid of N = 900 turns has a total magnetic flux of Φ = 1.33 x 10^-7Wb through its air core (no relative permeability required here) when the coil current is 100mA. If the flux takes up t = 75ms to grow from zero to max, calculate:
- the Inductance of the coil
- the counter-emf (self-induced emf) that is being created during that flux growth
Another way of calculating the Inductance of a coil is using the rate of magnetic flux per current change (dΦ/di) times the number N of coils. Using this equation the Inductance is:
The self-induced emf in the coil caused by the magnetic flux change is:
The negative sign shows us that the induced emf acts in the opposite sense!
Let's now also consider a hollow air-corded inductor coil of N = 500 turns of wire which produces a magnetic flux of Φ = 10mWb when a DC current of I = 10A passes through it. Calculate:
- the Self-Inductance of the coil
- The self-induced emf after a time of t = 10ms
The Self-Inductance is simply:
Therefore the self-induced emf is:
A very simple example, just to show you that only the "max" value matters!
Magnetic (and Electric) Energy Density
Let's now get into a somehow different topic, which has to do with magnetic and electric energy and more specifically the density of it...
Let's consider a region of space with a magnetic field of T = 1 x 10^-2T and a electric field of E = 2x10^6 V/m. Calculate the total/combined energy density of the electric and magnetic fields.
The energy density of the electric field can be calculated using:
The magnetic energy density is:
The net energy density is the sum of each energy and so:
Another complete, solved (and almost identical) example can be found at:
Let's now get into circuits, starting off with R-L (or L-R) circuits!
Let's consider a coil with inducatance L = 40mH and resistance R = 2Ω that is connected in series with a V = 20V DC power supply and "separated" by a switch. Let's calculate the:
- steady state (max) current
- time constant (τ)
- transient time
- induced emf (ε) after 10ms
- current after one time constant (after closing a switch).
The maximum current that can flow through a LR series circuit is known as steady state current and can be calculated using Ohm's law as:
The time constant (τ) in a RL series circuit can be calculated by:
The transient time for RL series circuit is approximately equal to 5 times the transient time and so:
Using the equation that we covered in the series/article we can find the emf/voltage after 10ms being:
The current after t = τ can be found using the corresponding equation as:
In this example we will now calculate the current without using the equations, by using a table of percentage that can be found at:
Let's consider a simple R-L circuit with an inductance of L = 1H, resistance of R = 5Ω and energy source of V = 10V.
Let's calculate the:
- maximum / steady state current
- time constant (τ)
- current after t = 0.5 τ
- current after t = τ
- current after t= 2τ
Using Ohm's law we have:
The time constant is:
The current after 0.5τ will have reached 40% of it's final/ultimate value (by taking a look on the table) and so is:
Using the table we see that the current will reach 63.2% of it's maximum value after τ seconds.
After t = 2τ the curent will reach 86.5% of it's final value which is:
Note: After t = 5τ the current is not exactly I, but 99.3% of the max value!
Let's now also get into a L-C circuit...Yeh, only one :P
Consider an oscillating LC circuit made of an 2μH inductor and 10nF capacitor. The maximum charge of the capacitor is 0.4μC. Let's find:
- The total energy of the circuit
- The absolute values of charge in the capacitor and current in the inductor the instant when 1/4 of the total energy is electric energy in the capacitor.
Such circuits are very easy to play with, cause everything has to do with energies...
Because of the conservation of energy and cause no energy is being lost as heat in a resistor, the total energy in the circuit stays the same and can be found at any instant of the oscillation. This means that the total energy can be found using the maximum charge of the capacitor, maximum current in the inductor, or even as a sum of the individual energies.
The maximum energy using the maximum charge of the capacitor is:
Knowing that the energy remains constant the magnetic energy will be 3/4 of the total energy, cause 1/4 is already being stored in the capacitor.
Knowing the inductance, the current flowing in the circuit/inductor (in series circuits the current is the same for all the components) can be found easily now as:
The absolute value of the capacitor charge can be calculated similarly as:
Any case can be calculated in a similar way!
Mathematical equations that I had in this post where drawn using quicklatex!
Previous posts about Electromagnetism
Getting into Electromagnetism -> electromagnetim, electric charge, conductors, insulators, quantization
Coulomb's law with examples -> Coulomb's law, superposition principle, Coulomb constant, how to solve problems, examples
Electric fields and field lines -> Electric fields, Solving problems around Electric fields and field lines
Electric dipoles -> Electric dipole, torque, potential and field
Electric charge and field Exercises -> examples in electric charges and fields
Electric flux and Gauss's law -> Electric flux, Gauss's law
Applications of Gauss's law (part 1) -> applying Gauss's law, Gauss applications
Applications of Gauss's law (part 2) -> more Gauss applications
Electric flux exercises -> examples in electric flux and Gauss's law
Electric potential energy -> explanation of work-energy, electric potential energy
Calculating electric potentials -> more stuff about potential energy, potential, calculating potentials
Equipotential surfaces and potential gradient -> Equipotential surface, potential gradient
Millikan's Oil Drop Experiment -> Millikan's experiment, electronvolt
Cathode ray tubes explained using electric potential -> cathode ray tube explanation
Electric potential exercises (part 1) -> applications of potential
Electric potential exercises (part 2) -> applications of potential gradient, advanced examples
Capacitors (Condensers) and Capacitance -> Capacitors, capacitance, calculating capacitance
How to solve problems around Capacitors -> combination, solving problems, simple example
Electric field energy and density -> Electric field energy, energy density
Dielectric materials -> Dielectrics, dielectric constant, permittivity and strength, how to solve problems
Electric capacitance exercises -> examples in capacitance, energy density and dielectrics
Current, resistance and EMF:
Electric current -> Electric current, current density
Electrical resistivity and conductivity -> Electrical resistivity, conductivity, thermal coefficient of resistivity, hyperconductivity
Electric resistance -> Resistance, temperature, resistors
Electromotive Force (EMF) and Internal resistance -> Electromotive force, internal resistance
Power and Wattage of Electronic Circuits -> Power in general, power/wattage of electronic circuits
Electric current, resistance and emf exercises -> exampes in all those topics
Direct current (DC) circuits:
Resistor Combinations -> Resistor combinations, how to solve problems
Kirchhoff's laws with applications -> Kirchhoff's laws, how to solve problems, applications
Electrical measuring instruments -> what are they?, types list, getting into some of them, an application
Electronic circuits with resistors and capacitors (R-C) -> R-C Circuit, charging, time constant, discharging, how to apply
RC circuit exercises -> examples in Kirchhoff, charging, discharging capacitor with/without internal resistance
Magnetic field and forces:
Magnetic fields -> Magnetism, Magnetic field
Magnetic field lines and Gauss's law of Magnetism -> magnetic field lines, mono- and dipoles, Flux, Gauss's law of magnetism
The motion of charged particles inside of a magnetic field -> straight-line, spiral and helical particle motion
Applications of charged particle motion -> CERN, Cyclotrons, Synchrotrons, Cavity Magetron, Mass Spectrometry and Magnetic lens
Magnetic force applied on Current-Carrying Conductors -> magnetic force on current-carrying conductors/wires, proofs
Magnetic force and torque applied on current loops (circuits) -> magnetic force on current loops, magnetic moment and torque
Explaining the Physics behind Electromotors -> tesla, history and explaining the physics behind them
Magnetic field exercises -> examples in magnetic force, magnetic flux, particle motion and forces/torque on current-carrying conductors
Magnetic field sources:
Magnetic field of a moving charged particle -> moving charge, magnetic field, force between parallel charged particles
Magnetic field of current-carrying conductors -> magnetic field of current, Biot-Savart law
Force between parallel conductors and the magnetic field of a current loop-> force between parallel conductors, magnetic field of current loop
Ampere's law and Applications -> Ampere's law, applications
Magnetic materials -> Magnetic materials, classification and types, material examples
Displacement current -> Displacement current, Extension of Ampere's law
Exercises in Magnetic field sources -> examples all around magnetic field sources
Electromagnetic Induction and Faraday's law -> Electromagnetic Induction, Experiments, Faraday's law
Motional Electromotive Force (Emf) -> Motional Emf, Faraday's law and motional emf, generalization
Lenz's law and Induced Electric fields -> Lenz's law, Induced Electric Fields
Eddy Currents and Applications -> Εddy currents, applications (brakes, testing, others)
Maxwell's equations -> What they are, each equation analyzed separately
Electromagnetic Induction exercises -> examples all around Electromagnetic Induction
Mutual and Self Induction:
Mutual Inductance -> Mutual Inductance, applications
Self Induction -> Self Induction, Lenz's law, Inductance of a Coil
Magnetic Energy Density -> Energy stored in a magnetic field (or inductor), Magnetic energy density, Coaxial Cable Inductance Example
R-L circuits -> R-L circuit energizing, de-energizing, Characteristic time constant
L-C circuits -> L-C circuit, oscillations, energy cases, applications
R-L-C circuits -> R-L-C circuit, oscillation, applications
And this is actually it for today's post and I hope that you learned how to apply all the things that we covered in actual mathematical problems! After my vacation we will continue with Alternating current :) Yeh, I know I'm in vacation all the Summer. Next up: "Limnos". Articles about it will start by Monday ;)