inductance benchmark companies inc po box 473768 aurora co 80047
TRANSCRIPT
![Page 1: INDUCTANCE Benchmark Companies Inc PO Box 473768 Aurora CO 80047](https://reader033.vdocument.in/reader033/viewer/2022052701/56649c725503460f94923050/html5/thumbnails/1.jpg)
INDUCTANCE
Benchmark Companies IncPO Box 473768Aurora CO 80047
![Page 2: INDUCTANCE Benchmark Companies Inc PO Box 473768 Aurora CO 80047](https://reader033.vdocument.in/reader033/viewer/2022052701/56649c725503460f94923050/html5/thumbnails/2.jpg)
DEFINED
When a length of wire is formed onto a coil, it becomes a basic inductor
![Page 3: INDUCTANCE Benchmark Companies Inc PO Box 473768 Aurora CO 80047](https://reader033.vdocument.in/reader033/viewer/2022052701/56649c725503460f94923050/html5/thumbnails/3.jpg)
DEFINED
Magnetic lines of force around each loop in the winding of the coil effectively add to the lines of force around the adjoining loops, forming a strong electromagnetic field within and around the coil
![Page 4: INDUCTANCE Benchmark Companies Inc PO Box 473768 Aurora CO 80047](https://reader033.vdocument.in/reader033/viewer/2022052701/56649c725503460f94923050/html5/thumbnails/4.jpg)
DEFINED
A inductor is a device which stores energy in a magnetic field
![Page 5: INDUCTANCE Benchmark Companies Inc PO Box 473768 Aurora CO 80047](https://reader033.vdocument.in/reader033/viewer/2022052701/56649c725503460f94923050/html5/thumbnails/5.jpg)
DEFINED
Inductor consists of a coil of wire, usually around a metallic or ferromagnetic core which creates an electromagnet
![Page 6: INDUCTANCE Benchmark Companies Inc PO Box 473768 Aurora CO 80047](https://reader033.vdocument.in/reader033/viewer/2022052701/56649c725503460f94923050/html5/thumbnails/6.jpg)
DEFINED
A current through an inductor creates a magnetic field around the coil which resists any changes in current
![Page 7: INDUCTANCE Benchmark Companies Inc PO Box 473768 Aurora CO 80047](https://reader033.vdocument.in/reader033/viewer/2022052701/56649c725503460f94923050/html5/thumbnails/7.jpg)
DEFINED
The unit of inductance is the henry (H), defined as the inductance when one ampere per Second through the coil, induces one volt across the coil
l
ANL
2
![Page 8: INDUCTANCE Benchmark Companies Inc PO Box 473768 Aurora CO 80047](https://reader033.vdocument.in/reader033/viewer/2022052701/56649c725503460f94923050/html5/thumbnails/8.jpg)
DEFINED
The unit of inductance is the henry (H), defined as the inductance when one ampere per Second through the coil, induces one volt across the coil
l
ANL
2
N= Number of Turnsµ = dielectric constantA = cross-sectional area of the coill = length of the coil
![Page 9: INDUCTANCE Benchmark Companies Inc PO Box 473768 Aurora CO 80047](https://reader033.vdocument.in/reader033/viewer/2022052701/56649c725503460f94923050/html5/thumbnails/9.jpg)
DEFINED
Schematic Symbols
Fixed Inductor Variable
• A couple of symbols for the inductor are illustrated below
L1
1.0mH
L2
10mH-VARKey = A
50%
![Page 10: INDUCTANCE Benchmark Companies Inc PO Box 473768 Aurora CO 80047](https://reader033.vdocument.in/reader033/viewer/2022052701/56649c725503460f94923050/html5/thumbnails/10.jpg)
INDUCTOR TYPES
Toroidal core inductor Axial Lead Variable Inductor
![Page 11: INDUCTANCE Benchmark Companies Inc PO Box 473768 Aurora CO 80047](https://reader033.vdocument.in/reader033/viewer/2022052701/56649c725503460f94923050/html5/thumbnails/11.jpg)
Rules of Inductor Behavior
The current and voltage relationship in an inductor is
If the current isn’t changing, then the voltage change across the inductor is zero
t
iL
dt
diLtv
)(
![Page 12: INDUCTANCE Benchmark Companies Inc PO Box 473768 Aurora CO 80047](https://reader033.vdocument.in/reader033/viewer/2022052701/56649c725503460f94923050/html5/thumbnails/12.jpg)
Rules of Inductor Behavior
An inductor is a short circuit to DC The current through an inductor cannot
change instantaneously If current changed quickly, then we might
have infinite voltage Contradicts conservation of energy
t
iL
dt
diLtv
)(
![Page 13: INDUCTANCE Benchmark Companies Inc PO Box 473768 Aurora CO 80047](https://reader033.vdocument.in/reader033/viewer/2022052701/56649c725503460f94923050/html5/thumbnails/13.jpg)
Example Problem 1What are the values of I and V, the current through and voltage across the inductor?
The easier value to find is the voltage V. In this case, the current through the inductor isn’t changing, so the voltage must be 0 V. So V = 0 V
In DC conditions, an inductor acts like a short circuit – so we need to find the current through the resistor and it will be the same as the current through the inductor.
mAk
V
R
VI 5
1
5
![Page 14: INDUCTANCE Benchmark Companies Inc PO Box 473768 Aurora CO 80047](https://reader033.vdocument.in/reader033/viewer/2022052701/56649c725503460f94923050/html5/thumbnails/14.jpg)
INDUCTOR CODEUse the color code guide in your handout as a means to
Identify the value of the inductor.
![Page 15: INDUCTANCE Benchmark Companies Inc PO Box 473768 Aurora CO 80047](https://reader033.vdocument.in/reader033/viewer/2022052701/56649c725503460f94923050/html5/thumbnails/15.jpg)
RL TIME CONSTANT
The RL Time Constant is the time it takes, in a series resistor inductor circuit, for current to rise to 63.2% or fall to 36.8% of the peak voltage value of the circuit. When five of these time constants occur, the inductor will be fully discharged. The formula below can be used to predict this value.
RLt / t = Time in secondsR = Resistance in OhmsL = Inductance in Henry’s
![Page 16: INDUCTANCE Benchmark Companies Inc PO Box 473768 Aurora CO 80047](https://reader033.vdocument.in/reader033/viewer/2022052701/56649c725503460f94923050/html5/thumbnails/16.jpg)
RL TIME CONSTANT
The current across an inductor cannot change instantaneously because a finite time is required to move charge from one point to another (limited by circuit resistance)
RLt / t = Time in secondsR = Resistance in OhmsL = Inductance in Henry’s
![Page 17: INDUCTANCE Benchmark Companies Inc PO Box 473768 Aurora CO 80047](https://reader033.vdocument.in/reader033/viewer/2022052701/56649c725503460f94923050/html5/thumbnails/17.jpg)
RL TIME CONSTANT example
With a 1kΩ resistor and a 1mH inductor are placed in series, what is the time constant of the circuit and how long will it take to fully discharge the inductor?
Discharge Time = 1us x 5Full Charge Time = 5us
Time for DischargeTime Constant Calculationt =L/Rt=1mH/1kΩ t =.001/1000t=1us
![Page 18: INDUCTANCE Benchmark Companies Inc PO Box 473768 Aurora CO 80047](https://reader033.vdocument.in/reader033/viewer/2022052701/56649c725503460f94923050/html5/thumbnails/18.jpg)
The first cursor proves that at 1us the current is 6.32V
The second cursor is showing that after 5 time constants the inductor represents a short circuit.
RL TIME CONSTANT GRAPHIC REPRESENTATION
![Page 19: INDUCTANCE Benchmark Companies Inc PO Box 473768 Aurora CO 80047](https://reader033.vdocument.in/reader033/viewer/2022052701/56649c725503460f94923050/html5/thumbnails/19.jpg)
When a DC voltage source is connected to the inductor, voltage is maximum across the inductor because of the magnetic field caused by the maximum rate of change of current in the circuit.
Note: at t = 0 seconds •Current is 0 Amps•Voltage is Maximum Volts
THEORY
/tEeVL
)1( /)0(
teII tL
![Page 20: INDUCTANCE Benchmark Companies Inc PO Box 473768 Aurora CO 80047](https://reader033.vdocument.in/reader033/viewer/2022052701/56649c725503460f94923050/html5/thumbnails/20.jpg)
THEORYAs the magnetic field “relaxes” due to the continuous DC, current begins to flow through the inductor. When this occurs, the voltage across the inductor begins to decrease and current through the inductor begins to rise.
/tEeVL
)1( /)0(
teII tL
![Page 21: INDUCTANCE Benchmark Companies Inc PO Box 473768 Aurora CO 80047](https://reader033.vdocument.in/reader033/viewer/2022052701/56649c725503460f94923050/html5/thumbnails/21.jpg)
THEORYEventually the inductor represents a short circuit. In an ideal inductor the voltage drop becomes 0 Volts and the current through the inductor becomes maximum.
Note: at t = infinity seconds •Current is Maximum Amps•Voltage is 0 Volts
/tEeVL
)1( /)0(
teII tL
![Page 22: INDUCTANCE Benchmark Companies Inc PO Box 473768 Aurora CO 80047](https://reader033.vdocument.in/reader033/viewer/2022052701/56649c725503460f94923050/html5/thumbnails/22.jpg)
Series and Parallel Inductors Inductors in Series
With several Inductors in series, they all act together to affect the current
neq LLLLL ...321
![Page 23: INDUCTANCE Benchmark Companies Inc PO Box 473768 Aurora CO 80047](https://reader033.vdocument.in/reader033/viewer/2022052701/56649c725503460f94923050/html5/thumbnails/23.jpg)
Series and Parallel Inductors Inductors in Parallel
With several Inductors in parallel, we have to split the current, just like in resistors
neq LLLLL
1...
1111
321
![Page 24: INDUCTANCE Benchmark Companies Inc PO Box 473768 Aurora CO 80047](https://reader033.vdocument.in/reader033/viewer/2022052701/56649c725503460f94923050/html5/thumbnails/24.jpg)
End of Presentation