lecture 1

15
ATIADE Mads Dyrmann Larsen Techinal IT student [email protected] 1 | 2012

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Page 1: Lecture 1

ATIADE

Mads Dyrmann Larsen

Techinal IT student

[email protected]

1 | 2012

Page 2: Lecture 1

Exam:

• Oral examn with known questions, but no preparation at the examn. • Grades are given in the 7 scale

2 | 2012

Page 3: Lecture 1

Example of a process control system

The skecth shows the transistion from a process to our processor and the

transistion from the processor to processor to a process.

Example: sound

The sound is sensed by a microphone diaphgram(1), it is converted to an electric

signal (2), which is transmitted through a cable (3). The signal is amplified (4) and

afterwards converted to a digital signal (5) that is lead into a signal processor.

The same goes the other way from processor to speaker (10)

3 | 2012

Page 4: Lecture 1

Example: Capacitiv humidity sensor (Philips H1)

4 | 2012

Page 5: Lecture 1

Example: Capacitive proximity sensor

http://www3.sea.siemens.com/step/pdfs/sensors.pdf

The sensing surface of a capacitive sensor is formed by two concentrically

shaped metal electrodes of an unwound capacitor. When an object nears

the sensing surface it enters the electrostatic field of the electrodes and

changes the capacitance in an oscillator circuit. As a result, the oscillator

begins oscillating. The trigger circuit reads the oscillator’s amplitude and

when it reaches a specific level the output state of the sensor changes. As

the target moves away from the sensor the oscillator’s amplitude

decreases, switching the sensor output back to its original state.

Standard targets are specified

for each capacitive sensor. The

standard target is usually

defined as metal and/or water.

Capacitive sensors depend on

the dielectric constant of the

target. The larger the dielectric

number of a material the easier

it is to detect. The following

graph shows the relationship of

the dielectric constant of a target

and the sensor’s ability to detect

the material based on the rated

sensing distance (Sr).

The following table shows the dielectric constants of some

materials. If, for example, a capacitive sensor has a rated

sensing distance of 10 mm and the target is alcohol, the

effective sensing distance (Sr) is approximately 85% of the

rated distance, or 8.5 mm.

One application for capacitive proximity sensors is level

detection through a barrier. For example, water has a much

higher dielectric than plastic. This gives the sensor the ability to

“see through” the plastic and detect the water.

5 | 2012

Page 6: Lecture 1

Example: Resistance thermometers

Platinum resistance thermometers (PRTs) offer excellent accuracy over a wide temperature range (from -200 to +850 °C).

Standard Sensors are available from many manufacturers with various accuracy specifications and numerous packaging

options to suit most applications. Unlike thermocouples, it is not necessary to use special cables to connect to the sensor.

The principle of operation is to measure the resistance of a platinum element. The most common type (PT100) has a

resistance of 100 ohms at 0 °C and 138.4 ohms at 100 °C. There are also PT1000 sensors that have a resistance of 1000

ohms at 0 °C.

The relationship between temperature and resistance is approximately linear over a small temperature range: for example, if

you assume that it is linear over the 0 to 100 °C range, the error at 50 °C is 0.4 °C. For precision measurement, it is necessary

to linearise the resistance to give an accurate temperature. The most recent definition of the relationship between resistance

and temperature is International Temperature Standard 90 (ITS-90).

http://www.picotech.com/applications/pt100.html

6 | 2012

Page 7: Lecture 1

Example: NTC Thermistor NTC=negative temperature coefficient

Source: EPCOS

Temperature dependence of resistance: The dependence of the resistance on temperature can be approximated by the following equation:

Where:

RT NTC resistance in Ω at temperature T in K

RR NTC resistance in Ω at temperature TR in K

T, TR Temperature in K

B B value, material-specific constant of the NTC thermistor

e Eulers number (~2,7183)

7| 2012

Page 8: Lecture 1

Example: Strain gauge

The strain gauge is connected into a Wheatstone Bridge circuit

with a combination of four active gauges (full bridge), two gauges

(half bridge), or, less commonly, a single gauge (quarter bridge).

In the half and quarter circuits, the bridge is completed with

precision resistors.

8 | 2012

Page 9: Lecture 1

Principals of different magnetic sensors

When V and ω are constant, it means that the formula is

changed to:

Each time a tooth is approaching and moving away

from the N-pole there is a change in the magnetic flux

in the windings around the magnet, thereby inducing

a voltage across the winding. The voltage amplitude

is proportional to the change in the flux and the

frequency of the voltage signal is proportional to the

rotational speed.

V

The power loss in the metal plate

changes the inductance of the

sensor which can be converted into

a voltage change.

Source: Measurement and Instrumentation principles, Allan S. Morris

Where K is constant. Larger distance means smaller L and thereby larger I

V = voltage, ω = angular frequency, L = inductance , I = current.

Magnetic body

9| 2012

Page 10: Lecture 1

Microphone

10 | 2012

Dynamic Microphones

A dynamic microphone takes advantage of electromagnet effects.

When a magnet moves past a wire (or coil of wire), the magnet

induces current to flow in the wire. In a dynamic microphone, the

diaphragm moves either a magnet or a coil when sound waves hit the

diaphragm, and the movement creates a small current.

Electret Microphone

Electret microphones are a special form of the

cendenser microphone, which eliminates the need

for a polarizing power supply by using a

permanently charged material´. The preamp circuit

uses an FET in a common source configuration. The

two-terminal electret capsule contains an FET which

must be externally powered by a a bias voltage

(~1.5-9V). The resistor sets the gain and output

impedance.

Condenser Microphones

A condenser microphone is essentially a capacitor,

with one plate of the capacitor moving in response

to sound waves. The movement changes the

capacitance of the capacitor, and these changes are

amplified to create a measurable signal. Condenser

microphones usually need a battery to provide a

(phantom) voltage(~11V-48V) across the capacitor.

Page 11: Lecture 1

MEMS microphones Over the last few years the MEMS(Micro Electro-Mechanical Systems) microphone

has grown to be a big competitor to the electret microphone. This is due to its very small size, compareable audio quality and often build-in ADC, which makes them very useful in devices like cell phones.

The mems microphones are often variants of the condenser microphone design.

11 | 2012

Page 12: Lecture 1

Magnetic proximity sensor

http://www3.sea.siemens.com/step/pdfs/sensors.pdf

Electromagnetic Coil and Metal Target

The sensor incorporates an electromagnetic coil which is used to detect the

presence of a conductive metal object. The sensor will ignore the presence

of an object if it is not metal.

Siemens BERO inductive proximity sensors are operated using

an Eddy Current Killed Oscillator (ECKO) principle. This type of

sensor consists of four elements: coil, oscillator, trigger circuit,

and an output. The oscillator is an inductive capacitive tuned

circuit that creates a radio frequency. The electromagnetic field

produced by the oscillator is emitted from the coil away from

the face of the sensor. The circuit has just enough feedback

from the field to keep the oscillator going.

When a metal target enters the field, eddy currents circulate

within the target. This causes a load on the sensor, decreasing

the amplitude of the electromagnetic field. As the target

approaches the sensor the eddy currents increase, increasing

the load on the oscillator and further decreasing the amplitude

of the field. The trigger circuit monitors the oscillator’s amplitude

and at a predetermined level switches the output state of the

sensor from its normal condition (on or off). As the target moves

away from the sensor, the oscillator’s amplitude increases. At a

predetermined level the trigger switches the output state of the

sensor back to its normal condition (on or off).

12 | 2012

Page 13: Lecture 1

Hall effect

Where K is the Hall constant.

The voltage V is in the horisontal

direction.

Where:

I is the current across the plate length,

B is the magnetic field

n is the density of charge carriers,

e is the electron charge (approx. 1.6 × 10−19 C)

d is the depth (thickness) of the plate

If an electric current flows through a conductor in a

magnetic field, the magnetic field exerts a transverse

force on the moving charge carriers which tends to

push them to one side of the conductor. This is most

evident in a thin flat conductor as illustrated. A buildup

of charge at the sides of the conductors will balance

this magnetic influence, producing a measurable

voltage between the two sides of the conductor.

Note that the direction of the current I in the diagram is

that of conventional current, so that the motion of

electrons is in the opposite direction.

The voltage across the plate can be calculated as:

As the plate doesn’t change, the formula can be

simplified to:

13 | 2012

Page 14: Lecture 1

I3GFV: Optisk fiber

The larger the pressure, the more light

dissaperears in the cladding which means

that less light is detedted.

no is the refractive index

In the air outside the fiber, n1 is

the refractive index in for the

kernal, n2 is the refractive index

for the cladding.

n1 ˃ n2 ˃ no

The refraction at change of the

mediums can be determined by

Snells law:

As long as 2 90, All the light

stay in the kernal.

Air to kernal:

Kernal to cladding:

14 | 2012

Page 15: Lecture 1

Smoke detector

Ionization Detectors: Ionization Chamber

An ionization chamber is very simple. It consists of two

plates with a voltage across them, along with a

radioactive source of ionizing radiation, like this:

The alpha particles generated by the americium have

the following property: They ionize the oxygen and

nitrogen atoms of the air in the chamber. To "ionize"

means to "knock an electron off of." When you knock

an electron off of an atom, you end up with a free

electron (with a negative charge) and an atom missing

one electron (with a positive charge).

The negative electron is attracted to the plate

with a positive voltage, and the positive atom is

attracted to the plate with a negative voltage

(opposites attract, just like with magnets). The

electronics in the smoke detector sense the

small amount of electrical current that these

electrons and ions moving toward the plates

represent.

When smoke enters the ionization chamber, it

disrupts this current -- the smoke particles attach

to the ions and neutralize them. The smoke

detector senses the drop in current between the

plates and sets off the horn.

http://home.howstuffworks.com/smoke3.htm

15 | 2012