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Acknowledgements
" #ould li$e to ac$no#ledge and t%an$ t%e man& people #%o %ave contributed to t%e re'
design and development of EE3. "n particular t%e )%air of t%e Department ofEngineering Professor *ran$ )%ang #as instrumental in providing t%e resources of staff
and funding necessar& to develop t%e ne# course.
Professor +reg Pottie developed t%e ne# lecture format and content of t%e course and
greatl& assisted in t%e development of t%e laborator& part.
Professor ,illiam -aiser provided valuable suggestions on t%e use of t%e " m&D/
device t%at %as been included in support of t%e laborator& portion of t%is course.
Dr. Mic%ael riggs is t%an$ed for %is generous insig%t into t%e c%anges t%at needed to be
made to improve t%e program based on %is eperience #it% t%e previous EE3.
Previous students of EE3 gave us man& suggestions t%at #e %ave attempted to include in
t%e re'design of t%is important "ntroduction to Electrical Engineering.4
*inall& " t%an$ t%e Elenco )orporation for t%e generous use of t%eir cop&rig%ted
materials.
'Prof Oscar Stafsudd 2012
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,ee$
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1
EQUIPMENT AND DEVICES
Introduction
6%e purpose of t%is laborator& is to provide t%e student #it% eperience in using t%e basic
measurement tools and an opportunit& to appl& t%ese tools to a term proCect. 6%e subCect
areas include@
1. Multi'meters2. *unction generators3.
Po#er supplies
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EE3 Laboratory Safety Course Certificate
F6E/> O56 6G"S P/+EH
S"+ /D D/6E 6G"S )E>6"*")/6E /D 65> " 6O ?O5> 8/O>/6O>?
6E/)G"+ /SS"S6/6 ,GE ?O5 G/7E S5))ESS*588? )OMP8E6ED 6GE
E)ESS/>? S/*E? )O5>SE(S!
" certif& t%at " %ave ta$en and passed t%e 5)8/ 8aborator& Safet& )ourse and all
necessar& additional safet& courses. " #ill abide b& t%e safet& reuirements for EE3
"ntroduction to Electrical Engineering4.
Date@ IIIIIIIIIIIIIIIIIIIIIIII
Student "D@ IIIIIIIIIIIIIIIIIIIIIIII
ame (Print ame )learl&!@ IIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIII
Signature@ IIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIII
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MultiMeters
6%e multiple function meter more commonl& referred to as t%e multi'meter is t%e mostbasic of electrical measurement devices. 6%ese meters occur in t#o basic t&pes@ t%e analog
multi'meter (/MM! and digital multi'meter (DMM!. /lt%oug% t%e t#o t&pes perform
similar measurements t%eir met%ods differ and t%eir limitations are uite different.
Analo! MultiMeters "AMMs#
FSee /ppendi for additional information.H
/t t%e %eart of all analog meters is a current measuring device (see *igures 1a and 1b!.
6%e meter #or$s as follo#s@ t%e current passing t%roug% a coil produces a torue due to
t%e magnetic field across t%e coil. 6%is torue t%en acts against a spring and moves anindicator %and. 6&pical meters reuire 10
'1to 10
'Aamperes to deflect t%e indicator %and to
full scale. 6%e mec%anism is generall& mec%anicall& delicate and does not li$e p%&sical
s%oc$s i.e. dropping. 6%e accurac& is in t%e order of A'10J. 6%e electrical euivalent
circuit is s%o#n in *igure 2 #%ere t%e resistance of t%e coil and its connections are lumped
into >i(t%e internal resistance of t%e meter!.
*"+5>E 1a@ //8O+ M586"'ME6E>
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>int. 6%erefore a meter
#ill %ave multiple values of >intto be selected.
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*"+5>E S)/8E
/n analog meter can also be used to measure current. 6o do t%is t%e meterQs terminals are
placed in series #it% t%e current to be measured (*igure A!. ote t%at if one does not #is%
to perturb t%e circuit b& t%e measurement process t%en t%e resistance >int s%ould ideall&
be 0 o%ms. Since t%is is not possible one must consider t%e effect of t%e >intresistance ont%e circuit. 6&picall& if >intRR t%e resistors in t%e circuit t%ere #ill be a negligible effect
on t%e accurac& of t%e measurement.
*"+5>E A@ )5>>E6 ME/S5>"+ )">)5"6
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Di!ital MultiMeters "DMMs#
FSee /ppendi ) for additional informationH
Digital multi'meters currentl& dominate t%e mar$et. 6%eir advantages over analog meters
include@
1. "ncreased accurac&. /nalog meters are t&picall& no better t%an a fe# percentaccurate. Even ver& lo# cost digital meters are 0.1J or better in accurac&.
2. Mec%anical ruggedness. /nalog meters %ave delicate mec%anical metermovements #%ic% tend to be easil& damaged b& dropping etc.
3. Gig%er input resistance t%an possible #it% analog meters. 6&pical values eceed109o%ms.
esistance is measured b& a DMM b& putting a precision constant current source at t%e
measuring terminals. 6%en a resistor connected at t%e terminals #ill produce a voltage
drop proportional to bot% t%e resistor value in o%ms and t%e current source in amperes. /
significant advantage of t%is met%od of resistance measurement over t%e /MM is t%at t%e
readout is linear as long as t%e current source remains ideal. 6%e 0'2 7 measurement meter
#it% a 1 micro'ampere current source becomes a 0'2 mega'o%m device. & c%anging t%e
value of t%e constant current source t%e range can be adCusted.
6%e measurement met%od emplo&ed b& DMMs is to compare t%e voltage to be measured
to internall& generated voltages. 6%e internal voltage is c%anged until a matc% of sufficient
accurac& is ac%ieved. ecause t%e eternal voltage to be measured is compared it is
possible to ma$e t%e effective input resistance reac% etremel& large values and t%erefore
not interfere #it% t%e accurac& of t%e measurement. 6&pical DMMs in t%e voltage
measurement mode %ave effective input resistances in t%e 10 to
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6#o basic digital measurement met%ods are used in most DMMs. 6%e& are (1! t%e
integrator met%od and (2! t%e successive approimation met%od. 6%e integrator met%od
compares t%e eternal voltage to be measured (7m! #it% t%e voltage on a capacitor. /constant current source is connected to t%e capacitor and a digital timer is simultaneousl&
started. 6%e voltage on t%e capacitor 7cK c #%ere is t%e c%arge on t%e capacitor in
coulombs and c is t%e capacitance in farads. 6%e c%arge at 6K0 is set to ;ero and t%e
c%arge at time 6 is .
*or a constant current " t%e c%arge at time 6 is K "6 and
t%erefore t%e voltage on t%e capacitor is given as 7cK "6). 6%e voltage 7c is a linear
function of time. ,%en t%e comparator circuit detects t%at 7cK 7m t%e timer is stopped.
6%e digital value of t%e time represents t%e voltage t%at #as measured. "n realit& t%e
measurement is a bit more complicated if capacitors are not perfect and suffer from
various problems. 6o minimi;e t%e non'ideal nature of capacitors t%e circuit actuall&
measures t%e time to c%arge t%e capacitor and t%en to disc%arge it in order to ma$e t%e
measurement more accurate. Suc% circuits easil& ac%ieve 11000 accurac&.
Successive approimation t&pes of DMMs can ac%ieve %ig%er accuracies and %ig% speeds.
"n t%is t&pe of digital meter voltages produced b& a digital to analog converter (D/)! are
compared seuentiall& #it% increasing accurac&. 6%e internal voltage is produced b&
c%anging t%e value of resistors s#itc%ed across a constant current source. 6%e internal
voltage starts at 7Ma."f t%e eternal voltage to be measured 7mis greater t%an 7Mat%en
t%e instrument displa&s over range4. "f t%e eternal voltage is smaller t%an 7Ma t%en t%e
internal voltage is c%anged to 7Ma 2.
6%e voltages eternal and internal are compared again. "f t%e eternal voltage is smaller
t%an 7Ma 2 t%en t%e internal voltage is reduced to 7Ma
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$unction %enerators
*unction generators are time dependent voltage sources. 6%e& fall into t#o distinct t&pes@analog and digital. ?ou #ill %ave an opportunit& to use and familiari;e &ourself #it% bot%
t&pes.
/nalog function generators of t%e simplest t&pe produce sinusoidal and suare #aves i.e.
#aves #%ose voltage as a function of time are given b& 7(t! K 70sin(Ut! in t%e case of
sine #aves or #aves t%at alternate bet#een 70#it% a minimum of rise and fall time (see*igure =!. *reuentl& triangular #ave forms are also available in analog function
generators. / triangular #ave rises linearl& for N70to L70and t%e falls linearl& from L70
to N70successivel&.
*"+5>E =@ //8O+ *5)6"O +EE>/6O>
6%ese #ave forms can easil& be produced b& relativel& simple analog circuits. More
comple #ave forms suc% as modulated or gated repetitive sine suare or triangular #ave
forms can also be easil& produced. Go#ever for arbitrar& functions of time one s%ould
use a digital function generator.
Digital function generators are based on Digital to /nalog )onverters (D/)s! as are some
digital multi'meters. / series of numbers stored in a memor& is sent seuentiall& into a
D/). 6%e D/)Qs output as a function of time is t%en determined b& t%e arra& of numbers
stored in t%e memor&. 6%e series of voltage outputs produced b& t%e D/) can be used to
approimate an& arbitrar& function limited onl& b& t%e speed of t%e D/) and t%e si;e of
t%e memor&. 6%is series can be repeated to give a repetitive function or occur as a single
occurrence.
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6%e " m&D/ %as suc% an arbitrar& #aveform generator included as one of its
functions. Eac% t&pe of function generator (analog and digital! %as its advantages and
disadvantages so bot% s&stems continue to be popular and in production.
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Po&er Su''lies
6%e laborator& is euipped #it% 6e$troni dual po#er supplies #%ic% %ave variable outputvoltages and current limits (*igure 9!. 6%ese supplies act as almost perfect voltage
sources. 6%at is t%e& suppl& a constant output voltage regardless of current demand up to
t%e pre'set current limit at #%ic% point t%e& be%ave as current sources suppl&ing a fied
current even into a s%ort circuit N ;ero o%msV
*"+5>E 9@ D) PO,E> S5PP8?
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(scillosco'es
Oscilloscopes allo# us to displa& time dependent #ave forms. 6%e original scopes4 #ereanalog devices. 6%e signal to be displa&ed #as amplified and t%e amplified signal #as
t%en used to displace an electron beam verticall&. 6%e displacement #as usuall&
accomplis%ed electrostaticall&. 6%e %ori;ontal pat% of t%e beam #as determined b& a
second amplifier circuit. 6%e %ori;ontal position #as commonl& a linear function of time.
6%us t%e beam of electrons #as positioned %ori;ontall& as a linear function of time and
verticall& b& t%e signal. 6%e electron beam struc$ a front surface of t%e cat%ode ra& tube
#%ere a p%osp%or surface #as present. 6%e electron impact caused t%e p%osp%or to
fluoresce (lig%t up brig%tl&!. 6%e #ave form as a function of time #as displa&ed.
6%is met%od #as a maCor step for#ard at t%e time allo#ing t%e engineer to visuali;e t%etime dependent voltage. /nalog oscilloscopes #ere emplo&ed from t%e 1:30Qs t%roug% t%e
end of t%e 20t%centur&. Digital tec%nolog& in t%e form of fast analog to digital converters
along #it% advances in displa& tec%nologies led to t%e digital oscilloscope #%ic% %as
become t%e dominant tec%nolog& toda&.
6%e t&pical digital oscilloscope still amplifies and per%aps conditions t%e signal. 6%e time
dependent signal is t%en converted to digital information b& an analog to digital converter
(/D)!. 6%e sampling rate is continuousl& deposited in a *"*OType equation here.(firstin N first out! memor&. 6%e memor& is a certain number of addresses long (t&picall&
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ecause t%e data is in digital form man& mat%ematical operations can be performed suc%
as averaging addition subtraction division etc. of t#o or more different #aveforms. 6%e
data can also be transferred to a removable memor& allo#ing t%e operator to furt%eranal&;e or arc%ive t%e data.
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1int t%e euivalent internal resistor. 6%e non'ideal voltagesource approac%es ZidealQ as >int\ 0.
F6%e on'"deal 7oltage Source is also called a 6%evenin SourceH
Current Sources
)urrent sources also occur in ideal and non'ideal t&pes. /n ideal current source delivers a
constant current no matter #%at voltage is reuired. 6%e& are usuall& s%o#n b& double
circles #it% an arro# s%o#ing t%e direction of t%e current. Occasionall& &ou ma& also see
a diamond s%ape for a current source particularl& on +erman and *renc% circuit diagrams.
on'ideal sources are usuall& represented b& an ideal source #it% an internal parallel
resistor.
V
V
*deal Voltage +our,e
V
V
Rint
-on*deal Voltage +our,e
Rint
* *
*deal Current +our,e
*
-on*deal Current +our,e
Rint
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2=
F6%e on'"deal )urrent Source is also called a orton SourceH
6%e non'ideal source approac%es ZidealQ as >int\ .
One can use a constant voltage source to simulate a nearl& ideal constant current source b&
placing a ver& large resistance in series i.e.
6%e current t%roug% t%e load resistor >8can be found as@
70K i ( >8L >S!.
6%erefore
" K 70 (>SL >8!
"f >S]] >8 t%en i ^70>S (a constant value providing >S]] >8!.
,e #ill not %ave &ou perform current source eperiments at t%is time because current
#easure#ents are the easiest way to destroy a #eter.
MultiMeter Measure)ents
1. Pic$ = resistors #it% different color codes. Measure t%eir values #it% &our DMMand /MM. )ompare t%eir stated values and tolerances (color code! #it% &our
measured multi'meter results.
,O>- SGEE6 GE>E@
>esistor _ Mar$ed DMM J Deviation /MM JDeviationMeasured Measured
>1 IIIIIIII IIIIIIII IIIIIIII IIIIIII IIIIIIII
>2 IIIIIIII IIIIIIII IIIIIIII IIIIIII IIIIIIII
>3 IIIIIIII IIIIIIII IIIIIIII IIIIIII IIIIIIII
>
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>A IIIIIIII IIIIIIII IIIIIIII IIIIIII IIIIIIII
>= IIIIIIII IIIIIIII IIIIIIII IIIIIII IIIIIIII
"s t%e error4 or deviation4 greater or less t%an t%e indicated tolerance`
/S,E> GE>E@
2. "f &ou loo$ at a standard list of 20J resistors available &ou #ill see 1000 o%msand 1A00 o%ms but not 1200 o%ms. ,%&` "f &ou loo$ at AJ resistors #ould t%e
results be different` ,%&` F/ listing of resistor values can be found on t%e #all of
t%e laborator&.H
/S,E> GE>E@
3. Pic$ t#o resistors t%at are approimatel& t#o orders of magnitude different i.e.1000 and 100000 or 22 and 2200 (See *igures 13 1- SGEE6 GE>E@
>1)olor )ode 7alue@ IIIIIIIIIIIIII >1Measured 7alue@ IIIIIIIIIIIIII
>2)olor )ode 7alue@ IIIIIIIIIIIIII >2Measured 7alue@ IIIIIIIIIIIIIII
b. Measure t%em in series and parallel connections.,O>- SGEE6 GE>E@
>Series7alue@ IIIIIIIIIIIIII >Parallel 7alue@ IIIIIIIIIIIIII
c. )ompare &our measurements #it% t%e calculated values. ote@ in series t%elarger value dominates t%e measurement.
,O>- SGEE6 GE>E@
> Series >esistance )alculated@ IIIIII Measured@ IIIIIII J difference IIIIIII
> Parallel >esistance )alculated@ IIIII Measured@ IIIIIII J difference IIIIIII
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d. "n t%e parallel connection #%ic% resistor dominates and #%&`/S,E> GE>E@
*"+5>E 13. M586"ME6E>S )OE)6ED
6O >ES"S6O> O P>O6O'O/>D
F8eft side@ /nalog Multimeter >ig%t side@ Digital MultimeterH
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2:
*"+5>E 1ES"S6O>S )OE)6ED " SE>"ES O P>O6O'O/>D
*"+5>E 1A. >ES"S6O>S )OE)6ED " P/>/88E8 O P>O6OO/>D
Source Measure)ents
6%e 6e$troni dual po#er suppl& &ou #ill be using can operate as a near ideal voltage
source and a near ideal current source (O6 simultaneousl&!.
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6o test a voltage source@
turn t%e current limit to full rig%t (cloc$#ise direction![ set t%e output to 10 volts[ set t%e DMM to read D) volts set t%e range to greater t%an 10 volts if available or auto'scale4 if t%e meter is so
euipped
Observe carefull& t%e small c%ange in t%e output voltage t%at #ill occur #%en t%e resistor
is connected. *rom t%e c%ange in t%is voltage calculate t%e internal resistance of t%e
voltage source. 6%e euivalent circuit is@
(6%e DMM input resistance is etremel& large compared to >V!
Measure t%e output voltage carefull& #it% t%e meter connected to t%e suppl&. 6%en
connect a 10 3A ,att resistor across t%e t#o output terminals #it% t%e po#er suppl& set
at approimatel& 10 volts. ote@ t%e resistor #ill dissipate energ& and get uite GO6VV
6a$e care not to burn &ourself. See *igure 1=. F6%e resistor ma& loo$ slig%tl& different.H
+
u
p
p
l
y
/
o
0
e
r
V
Rint
R&
1
M
M
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*"+5>E 1=. 10 OGM >ES"S6O> )OE)6ED
6O M586"ME6E> /D PO,E> S5PP8?
,O>- SGEE6 GE>E@
5nloaded voltage (i.e. O 10 O%m resistor!@ IIIIIIIIIIIIII
8oaded voltage (10 O%m resistor!@ IIIIIIIIIIIIII
7oltage s%ift@ IIIIIIIIIIIIIIIIIII
)alculate internal resistance@
o# eplore t%e problems represented b& a non'ideal voltage source. Set t%e output
voltage to about 10 volts. Put a 10 - resistor in line #it% t%e positive terminal. 6%is
combination simulates a non'ideal po#er suppl& (or source!. 6%e euivalent circuit %as
>int^ 10- .
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DMM Measure)ent
Set t%e po#er suppl& voltage to about 10 7. Measure t%e DMM D) voltage reading at t%epo#er suppl& terminals and also after t%e - SP/)E GE>E@
D) 7oltage at po#er suppl&@ IIIIIIIIIIIIIIIIIIIIIIIIIIIIII
D) 7oltage after - SP/)E GE>E@
FMeter set to 10 7H
D) 7oltage at po#er suppl&@ IIIIIIIIIIIIIIIIIIIIIIIIIIIIII
D) 7oltage after
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ote t%at t%e loading effect of t%e /MM is different on different scales. )an &ou eplain
t%is`
,O>- SP/)E GE>E@
6%is simple eperiment demonstrates t%e loading4 effect of t%e analog meter and #%& itQs
necessar& to be uite careful in simple voltage measurements.
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3MS 7pp K `
3. 6riangular ,ave@ >MS 7pp K `
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3A
Ti)e De'endent Measure)ents
6%is #ee$Qs eperiments #ill give &ou t%e opportunit& to learn t%e basic operations of an
oscilloscope and a function generator.
6urn on bot% t%e function generator (*igure 19! and oscilloscope (*igure 1!. )onnect
c%annel 1 input of t%e oscilloscope to t%e function generator signal out4. )onnect t%e
s&nc out4 of t%e function generator to t%e scopeQs c%annel 2 (,it% t%e digital generator
use t%e generatorQs )%annel 1 since t%e S&nc Out is onl& associated #it% )%annel 1.
Enable S&nc Out in t%e 5tilit& Mode!. Set t%e freuenc& to 100 G; #it% amplitude
some#%ere bet#een 1 7 and 10 7. Set t%e function generator mode to sine output
(sinusoidal #aves!. Press t%e auto scale button on t%e scope. ?ou s%ould observe a
sinusoidal #ave form on t%e displa& (*igure 1:!.
.*"+5>E 19a@ //8O+ Signal +enerator
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3=
*"+5>E 19b@ D"+"6/8 Signal +enerator (frontbac$!
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*"+5>E 1@ OS)"88OS)OPE
*"+5>E 1:@ S)OPE D"SP8/?"+ S"5SO"D/8 S"+/8
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6o understand t%e trigger function of t%e scope select t%e trigger control. /fter pressing
t%e upper'rig%t corner /utoSet4 button t%e trigger is internall& set b& t%e scope. ,%ile
t%is is a good start #e #is% to %ave more control. 6%erefore ta$e direct control b& firstselecting t%e trigger menu and setting t%e source to be c%annel 1. ,it% t%e trigger in
Edge4 mode t%e (trigger! 8evel4 $nob can no# be used to control t%e voltage level at
#%ic% t%e scope #ill start its measurement i.e. its time reference point or trigger point.
ote@ if a trigger voltage point is selected t%at is outside of t%e range of voltages on
c%annel 1 t%en t%e scope #ill not displa& ne# data and #ill indicate on t%e displa& not
triggered4 or #aiting for trigger4 etc.
6%e trigger level is noted on t%e displa& b& eit%er a line or an arro# #it% 6 net to it.
/dCust t%e trigger level to obtain an active displa&. 6%e displa& #ill no# sa& triggered4
or running4. /dCust t%e trigger level and note its effect on t%e position of t%e #ave formon t%e displa& screen.
ote t%e level control also allo#s t%e slope of t%e level to be observed. )%ange t%e slope
(or sense! from increasing to decreasing bac$ and fort% to note t%e effect on t%e displa&.
Set t%e trigger level about %alf#a& bet#een 0 and t%e maimum value of t%e #ave form.
o# adCust t%e voltage level of t%e function generator and note t%e position of t%e 04
time c%anges #it% amplitude and t%at as t%e voltage of t%e function generator gets small
t%e trigger #ill eventuall& fail to #or$.
o# c%ange t%e trigger input to c%annel 2 (s&nc output of t%e function generator!. ote
t%at t%e trigger #ill no# remain constant regardless of t%e magnitude of t%e sinusoidal
signal. 6%is is t%e prime reason for t%e use of a s&nc output of t%e function generator.
)%ange t%e mode of t%e function generator from sine to triangular and t%en suare. ote
eac% of t%ese #ave forms. 6%e actual voltage levels can be measured b& using t%e voltage
cursor function of t%e scope. 5sing t%e )5>SO> controls measure t%e 7pp amplitude of
a sinusoidal #ave i.e. t%e pea$'to'pea$ amplitude of t%e #ave.
5sing &our analog and digital multi'meters on t%e /) voltage settings measure t%e
voltage of t%e #ave form. )ompare t%e scope and multi'meter indicated voltages. Go# do
&ou eplain t%ese results`
o# c%ange t%e mode to suare and t%en triangular and repeat t%e eperiment.
6%e follo#ing are four sets of similar measurements comparing t%e DMM and /MM@
*irst t%e #aveforms are measured at lo# freuenc& (100 G;! and lo# level (A7pp! t%en
lo# freuenc& and %ig% level (207pp!. *ollo#ing t%ose pair of measurements &ou #ill
increase t%e freuenc& to A $G; and repeat t%e lo#' and %i'level measurements. *rom all
t%ese measurements &ou can observe t%e limitations of eac% instrument.
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3:
,O>- SGEE6 GE>E@
,ave Scope 7oltage Meter 7oltage (>MS! Difference ( J ! 7s )alc
*orm ()5>SO>! )alc DMM /MM DMM /MM
100 G; A 7pp 7rms 7rms 7rms 7rms 7rms
Sine@ IIIIIIII IIII IIIIIII IIIIIII IIIIIII IIIIIII
6riangle@ IIIIIIII IIII IIIIIII IIIIIII IIIIIII IIIIIII
Suare@ IIIIIIII IIII IIIIIII IIIIIII IIIIIII IIIIIII
"f t%ere are differences eplain@
/S,E> GE>E@
,O>- SGEE6 GE>E@
,ave Scope 7oltage Meter 7oltage (>MS! Difference ( J ! 7s )alc
*orm ()5>SO>! )alc DMM /MM DMM /MM
100 G; 20 7pp 7rms 7rms 7rms 7rms 7rms
Sine@ IIIIIIII IIII IIIIIII IIIIIII IIIIIII IIIIIII
6riangle@ IIIIIIII IIII IIIIIII IIIIIII IIIIIII IIIIIII
Suare@ IIIIIIII IIII IIIIIII IIIIIII IIIIIII IIIIIII
"f t%ere are differences eplain@
/S,E> GE>E@
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- SGEE6 GE>E@
,ave Scope 7oltage Meter 7oltage (>MS! Difference ( J ! 7s )alc
*orm ()5>SO>! )alc DMM /MM DMM /MM
A $G; A 7pp 7rms 7rms 7rms 7rms 7rms
Sine@ IIIIIIII IIII IIIIIII IIIIIII IIIIIII IIIIIII
6riangle@ IIIIIIII IIII IIIIIII IIIIIII IIIIIII IIIIIII
Suare@ IIIIIIII IIII IIIIIII IIIIIII IIIIIII IIIIIII
"f t%ere are differences eplain@
/S,E> GE>E@
,O>- SGEE6 GE>E@
,ave Scope 7oltage Meter 7oltage (>MS! Difference ( J ! 7s )alc
*orm ()5>SO>! )alc DMM /MM DMM /MM
A $G; 20 7pp 7rms 7rms 7rms 7rms 7rms
Sine@ IIIIIIII IIII IIIIIII IIIIIII IIIIIII IIIIIII
6riangle@ IIIIIIII IIII IIIIIII IIIIIII IIIIIII IIIIIII
Suare@ IIIIIIII IIII IIIIIII IIIIIII IIIIIII IIIIIII
"f t%ere are differences eplain@
/S,E> GE>E@
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,/7E*O>M
"f &ou reduce t%e timebase to approimatel& 2A0 millisecondsdivision &ou #ill be
undersampling t%e #aveform and &ou #ill observe #aveforms similar to *igure 21.
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,/7E*O>M
?our 6/mentor #ill %elp &ou displa& t%is effect. ecause of undersampling &our scope
is displa&ing a lo# freuenc& #aveform #%ic% does not eist and is an artifact of aliasing
(&uist!. *igures 22 and 23 s%o# t%e same results for sinusoidal #aves.
*"+5>E 22@ )O>>E)68? S/MP8ED S"5SO"D/8 ,/7E*O>M
*"+5>E 23@ ")O>>E)68? S/MP8ED S"5SO"D/8 ,/7E*O>M
6%e 6/ and class mentors #ill demonstrate t%e use of t%e curve tracer and current sources
to t%e class as time permits.
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/SD5)E>S MO56ED O P7) )O5P8E>S.
)onnect t%e s&nc output of t%e function generator to )%annel 1 of &our scope and set t%e
scope to trigger on )%annel 1 (6%is #ill be automaticall& done #%en &ou press t%e scopeQs
/utoSet button.! Select A $G; on t%e function generator and an output a level 3 7pp.
/lso ma$e sure t%e function generator is set to sine #aves. )ouple t%e t#o transducers
acousticall& b& placing a s%ort piece of P7) pipe bet#een t%em. 6%e pipe acts as a
#aveguide for t%e acoustic #aves. See *igure 2A.
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pK 1 +p and +pK +0 L "
#%ere +0is t%e dar$ conductance (1 >0!. 6%is device %as a +0^ 10=o%m. rig%t lig%t
i.e. sunlig%t #ill produce a resistance of ^1 - o%m or less.
*"+5>E 2=@ 8E*6@ PGO6OD"ODE )E6E>@ PGO6OD"ODE
>"+G6@ PGO6O')OD5)6O>
?our 6/ or mentor can %elp &ou displa& t%e lig%t and dar$ c%aracteristics (current vs.
voltage! of t%e device on t%e curve tracer. 6%e correct range of t%e setup is 0 N 20 7 and
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! and t%e device. 6%e
current can be calculated "DK 7> >. Measure t%e device in dar$ room lig%t and brig%t
lig%t using t%e lig%t bulb provided. ote@ in t%e dar$ a resistor value ^ 100 - o%ms is
appropriate and under brig%t lig%t 10 - or 1 - o%m.
Of t%e devices listed all t%e ot%ers are diodes t%at can eit%er generate lig%t (8EDs! or
absorb lig%t and generate current i.e. p%otodiodes p%oto transistors solar cells.
6%e current in a diode is a ver& non'linear and non's&mmetric function of voltage (see
*igures 29 and 2!. / reasonabl& accurate mat%ematical model of t%e current'voltagerelations%ip is@
"DK "0(e77t
N 1!
"n t%e for#ard direction i.e. 7 7t
"D^ "0 e77t
"n reverse 7 '7t t%en "D^ "0
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A0
*"+5>E 29@ PGO6OD"ODE D/>- *O>,/>D )G/>/)6E>"S6")
*"+5>E 2@ PGO6OD"ODE D/>- >E7E>SE )G/>/)6E>"S6")
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A1
*"+5>E 2:@ PGO6OD"ODE "885M"/6ED )G/>/)6E>"S6")
(*O>,/>D /D >E7E>SE!
ecause t%e currents in t%e for#ard and reverse directions are ver& different in si;e t%e
appropriate series resistors s%ould be c%anged. 6&picall& t%e reverse current is man&
orders of magnitude smaller t%an t%e for#ard current. Go#ever t%e po#er dissipation can
be large in t%e reverse direction because t%e voltage across t%e device can be uite large
(tens of volts!. "n t%e for#ard direction t%e t&pical voltage is in t%e order of a fraction of avolt for silicon devices and a fe# volts for 8EDs. 6%e suggested resistor values are in t%e
)urve 6racer "nstructions (See /ppendi /!. Observe t%e c%aracteristics.
ote@ t%e 8EDs actuall& emit lig%t in t%e for#ard direction. One possible future proCect for
&ou is to measure t%e lig%t output as a function of current andor voltage.
P,otodiodes
5nli$e 8EDs p%otodiodes are designed to absorb lig%t and convert it into electron %ole
pairs t%at generate a measurable voltage or current. / good circuit model for t%e
p%otodiode and its sc%ematic s&mbol are s%o#n %ere@
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A2
Mat%ematicall&
"DK "0(e77tN 1! ' "gen
ote@ "genis in a direction to for#ard bias t%e diode.
Solar cells are designed to convert lig%t (t&picall& solar radiation! to electrical po#er.
)onversion efficiencies for silicon are 10J AJ and t%e solar radiation level in sunn&
sout%ern )alifornia is about 100 m.#.cm2. P%otodiodes for t%e purpose of lig%t detection
are t&picall& small area devices t%at are designed to give %ig% sensitivit& and lo# noise.
Devices s%o#n in *igure 2= %ave areas in t%e order of 10'
to 10'=
cm2. 6%e values of
current are 10'=
N 10'3
amperes and care must be ta$en not to inCure t%ese devices. 6%e
correct settings for t%e devices can be found in t%e )urve 6racer "nstructions. Please use
t%e assistance of &our 6/ or mentor to operate t%e curve tracer (*igure 30!.
*"+5>E 30. )5>7E 6>/)E>
Solar cells are onl& used in t%e for#ard direction i.e. for generating po#er. e sure to
loo$ at t%e for#ard c%aracteristic of &our single solar cell in t%e dar$ and illuminated.
One of t%e simplest uestions t%at can be of interest is #%at load value i.e. resistance #ill
&ield t%e maimum po#er` /nd does t%is c%ange #it% illumination level`
P%otodiodes are used bot% in t%e for#ard biased and reverse biased conditions. e sure to
measure t%e p%otodiodes bot% dar$ and illuminated in bot% for#ard and reverse biased
conditions. )onsider t%e t#o common p%otodiode circuits@ P7 P). 6%e P7 mode
reuires one less component (no batter&! and P) mode responds faster to c%anges in lig%t.
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A3
,%at are t%e advantages of eac% circuit`
/S,E> GE>E@
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Aeverse t%e direction of t%e spin and note t%at t%e voltage reverses.
et investigate t%e device as a motor$ %&'() the s#all #otor can be da#aged if
#ore than * + C is applied directly across the #otor, so we ask that you always use
one of the big, white -. oh# power resistors in series with each #otor you use
Set t%e po#er suppl& to 04 volts output #it% t%e current $nob turned full& ),. )onnect
t%e motor in series #it% a (#%ite! 10 o%m po#er resistor to t%e po#er suppl&Qs output
terminals and connect &our DMM to measure t%e voltage across onl& t%e motor. Ma$e
sure t%e motor is mec%anicall& separated from an& gears if t%e gear bo is assembled so
t%e motor is free to turn #it%out being loaded b& an& gears. Set t%e s#itc% on t%e suppl&
to indicate /mps and t%en var& t%e suppl& voltage until t%e voltage &ou measure across
onl& t%e motor is set to eac% of t%e values in t%e follo#ing table. /t eac% setting note t%e
current indicated on t%e suppl&Qs /mp reading. ote t%at t%e motor s%aft spins rapidl& at
t%e %ig%er voltages. Measure t%e current b& separatel& measuring t%e voltage across t%e
resistor and using O%ms la#.
Stop measurement if t%e motor stops running at lo# voltages. ever appl& more t%an 37
across t%e motor.
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AA
,O>- SGEE6 GE>E@
Motor 7olts Motor )urrent
2.A IIIIIII
2.0 IIIIIII
1.A IIIIIII
1.0 IIIIIII
0.A IIIIIII
0.2 IIIIIII
0.1 IIIIIII
Plot &our results@
,%at voltage and current "o is reuired to Cust start t%e motor spinning`
6%is current "0represents t%e current reuired to simpl& turn over t%e motor in t%e absence
of doing eternal #or$. /s$ &our 6/mentor to demonstrate t%e effects on t%e current of a
load reuiring t%e motor to do eternal #or$.
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A=
0ee1 6 NI )yDAQ
5sing t%e Elvis program t%e " m&D/ can be launc%ed into modes in #%ic% it emulatesvarious laborator& devices. Details on %o# to do t%is can be found at t%e #ebsite@
###.ni.com#%ite'paper11MS.
,O>- SGEE6 GE>E@
1 $G; )&clic >MS
,ave 6e$ Scope Meter 7oltage J Difference (7s Scope!
(A 7pp! 7oltage DMM m&D/DMM DMM m&D/
Sine@ IIIIIIII IIIIIII IIIIIII IIIIIII IIIIIII
6riangle@ IIIIIIII IIIIIII IIIIIII IIIIIII IIIIIII
Suare@ IIIIIIII IIIIIII IIIIIII IIIIIII IIIIIII
"n particular does t%e M&D/ measurement of sine suare #aves and triangular #aves
be%ave t%e same or differentl& t%an t%e digital multi'meter` ,%&`
/S,E> GE>E@
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/ctivate t%e " m&D/ in (L+IS&scilloscope instrument. )onnect bot% t%e m&D/
and t%e 6e$troni scopes to t%e digital function generator. ote t%at t%e M&D/ analog
inputs are made t%roug% its edge connector and are differential (Cust li$e an Op/mp! #it%a non'inverting and a inverting terminal so &ou %ave to connect t#o #ires in order to
input t%e one signal. ?ou actuall& s%ould connect t%ree #ires for t%e one signal@
,%ic%ever input terminal (invertingnon'inverting! t%at &ou connect to &our signal
generatorQs ground () ground s%ield! &ou s%ould also connect t%at same terminal also
to t%e M&D/Qs analog ground terminal. (6%is minimi;es ground loop noise.!
)ompare t%e be%avior of t%e lab benc% 6e$troni and &our m&D/ oscilloscopes. Start
b& measuring t%e output of t%e function generator at about 1 $G; and amplitude of 1 N 10
7pp loo$ing at bot% sine and suare #aves. "ncrease t%e freuenc& of t%e function
generator to 1 -G; 10 $G; :: $G; ::: $G; and 1::: $G;. ote #%et%er t%e amplitudeof t%e sine #aves and particularl& t%e s%ape of t%e suare #aves remain constant. 6%e
digital function generator output is in fact constant over t%is freuenc& range so c%anges
in rise and fall time andor amplitude #it% freuenc& are t%e result of freuenc&
limitations in &our measuring devices. (6%e output of t%e analog function generator varies
some#%at over t%is freuenc& range.!
,O>- SGEE6 GE>E@
*reuenc& Oscilloscope >MS 7oltages IIIIIIIIIIIIIII
$G; Sine (6e$! Suare (6e$! Sine(m&D/! Suare (m&D/!
1 IIIIIIII IIIIIII IIIIIII IIIIIII
10 IIIIIIII IIIIIII IIIIIII IIIIIII
:: IIIIIIII IIIIIII IIIIIII IIIIIII
::: IIIIIIII IIIIIII IIIIIII IIIIIII
1::: IIIIIIII IIIIIII IIIIIII IIIIIII
Suare #ave response reuires a %ig%er freuenc& response from t%e measuring s&stemt%an sinusoidal #aves. /s &ou #ill see in t%e spectrum anal&;er eperiment suare #aves
can be t%oug%t of as being formed from a fundamental sinusoidal #ave #%ose period is
t%e same as t%e suare #ave #it% %ig%er freuenc& components (all odd %armonics! to
ma$e up t%e s%arp rise and flat top associated #it% t%e suare #ave.
6%erefore as &our measuring s&stem goes to its %ig% freuenc& limit t%e s%arp rise and
fall of t%e suare #ave #ill be lost due to t%e lac$ of t%ese %ig%er freuenc& components
being accuratel& displa&ed. Plot t%e sinusoidal freuenc& response versus freuenc& for
t%ese t#o oscilloscopes.
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A
/S,E> GE>E@
,e define t%e upper freuenc& response of a s&stem to be t%e point at #%ic% t%e amplitude
decreases to 90.9J ('3 d!. 5sing t%is criterion can &ou estimate t%e freuenc& response
of t%e m&D/ and t%e 6e$troni oscilloscopes` Discuss.
/S,E> GE>E@
*rom t%ese eperiments &ou #ill observe t%at t%e combination of a laptop computer and a
" m&D/ can emulate t%e common functions of a standalone multi'meter or
oscilloscope.
6%e " m&D/ #ill also operate as a function generator. Put t%e device in function
generator mode and test its output using t%e 6e$troni oscilloscope. 6est various
#aveforms suc% as sine suare and triangular outputs.
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A:
ote t%at t%e generator can also be used to generate arbitrar& #aveforms. 6%is #ill be
useful for t%e various proCects t%at &ou #ill c%oose to #or$ on. "n &our outside time
please eamine t%is option of generating arbitrar& #aveforms.
S'ectru) Analy*er Mode
Put t%e " m&D/ in spectrum anal&;er mode called a D&namic Signal /nal&;er4. 5se
t%e function generator to produce 1 $G; suare #aves of about 1 volt amplitude. /nal&;e
t%e spectrum of t%is suare #ave. )ompare t%e freuenc& components and t%eir
amplitudes to t%eor&. 6%at is onl& odd %armonics s%ould appear (1 $G; 3 $G; A $G;
etc.! and t%e ratio of t%e various %armonic amplitudes to t%at of t%e fundamental s%ould be
1 #%ere is t%e %armonic (1@ 13 @ 1A @ 19 @ W etc.!.
ote again@ t%e d&namic signal anal&;er can displa& t%e data in bot% a linear andlogarit%mic manner called d (decibel! defined as a ratio of po#ers@
ell K log10Po#er Po#erreference
d K 10 log10Po#er Po#erreferenceK 20 log107 7reference
6a$e t%e data bot% linearl& and logarit%micall&. 6%e logarit%m displa& gives greater detail
over a #ide d&namic range and is t%erefore commonl& used in engineering.
Set t%e **6 settings *re Span to 20 $G; *reuenc& Displa& 5nits to d and set t%e
Scale Settings Scale to Manual (Ma K 0 Min K 'un t%en clic$ t%e lo#er'left corner bo )ursors On4 drag t%e das%ed vertical green line (on t%e left side of t%e
displa&! %ori;ontall& until it snaps onto t%e first %armonic t%en drag t%e remaining second
das%ed vertical line to snap respectivel& on eac% of t%e %ig%er %armonics N one b& one.
Eac% time (snapped onto eac% of t%e %ig%er %armonics! note and record t%e value on t%e
left middle indicator in green as dd7rms (delta d!.
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=0
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=1
,O>- SGEE6 GE>E (S5/>E ,/7E //8?S"S!@
n 20 log(7n 71!Kdn'd1 20log(1n! nKodd[ 'inf nKeven
Garmonic >atio in d (n't% 1st! 6%eor& .
1 0 0
2
3
epeat t%e process #it% a triangular #aveform. )ompare t%e results to t%e t%eoretical
values.
,O>- SGEE6 GE>E (6>"/+58/> ,/7E //8?S"S!@
n 20 log(7n 71!Kdn'd1 20log(1n2! nKodd[ 'inf nKeven
Garmonic >atio in d (n't% 1st! 6%eor& .
1 0 0
2
3
EME6 SE6'5P
*"+5>E 32@ )8OSE'5P SGO,"+ 8ED /D SE>"ES >ES"S6O>
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=:
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90
et measure t%e lig%t output vs. device current. Put a single cell solar cell net to t%e
8ED. )onnect a multi'meter to t%e solar cell. 5se t%e meter in current mode4. See t%e
circuit diagram belo#. Put a s%ield over &our set up to avoid t%e effects of t%e laborator&lig%ts. 6%e 8ED is connected as before.
elo# is a picture of an /MM in current mode connected to a solar cell. ote@ it is asingle cell rated at h volt
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91
elo# see t%e set'up for measuring t%e lig%t output of a 8ED.
*"+5>E 3E 3A. )/>DO/>D O 5SED /S 8"+G6 SG"E8D
O6E@ a Cac$et can also serve t%is purpose.
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92
Measure t%e current from t%e solar cell #%ic% is linear in lig%t intensit& as a function of
8ED current. Put t%e /MM in current mode and on t%e 2.A m/ scale.
,O>- SGEE6 GE>E@
7olts (across 1-'o%m resistor! "Solar )ell "8ED
0.0 IIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIII
1.0 IIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIII
2.0 IIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIII
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93
Plot t%e solar cell current i.e. t%e lig%t output vs. t%e 8ED current.
/t t%is point &ou %ave demonstrated t%at t%e lig%t output of a 8ED is a linear function of
t%e current in t%e device. ,e s%all use t%is fact to test t%e be%avior of anot%er $ind of
p%oto'detector t%e p%otoconductor. 6%e p%otoconductor resistance #ill be measured b& a
multi'meter in t%e resistance measuring4 mode. >epeat t%e 8ED'solar cell eperiments
replacing t%e solar cell #it% t%e p%otoconductor. Measure t%e resistance of t%e
p%otoconductor as a function of 8ED current t%at is t%e 8ED output. 6%e p%otocell s%ouldCust $iss4 t%e 8ED to ensure proper alignment.
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9P%otoconductor "8ED
IIIIIIII0.0 IIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIII
IIIIIIII1.0 IIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIII
IIIIIIII2.0 IIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIII
IIIIIIII
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9A
Plot t%e p%otoconductor resistance vs. "8ED.
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9=
Plot t%e reciprocal of t%e p%otoconductor resistance vs "8ED.
et #ee$ (=! #e s%all eplore t%e use of a 8ED lig%t source a lig%t detector and its
circuitr& P Cunction p%otoconductor and p%ototransistor for@
t%e measurement of position transmission of information (bot% digital and analog!
and #%atever else &ou need to eplore for &our proCect
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99
Acoustic De+ices Pro9ects
*or t%is proCect &ou #ill be provided #it% broadband spea$ers4 and narro# band
(ultrasonic! transducers. 6%e laborator& also #ill %ave acoustic #aveguides (P7) pipe!
and couplers bends and special slip fittings. Pipes of h and 1 meter in lengt% #ill be
available. elo# is t%e picture of t&pical devices available for t%is proCect.
*"+5>E 3=. /)O5S6") DE7")ES
"n t%e picture Ftop to bottomH #e s%o#@ 1 m pipe h m pipe m pipe slip fittings
#ideband transducer narro# band transducer :0j bend E 39. 7">65/8 ODE "S6>5ME6
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9
*ind t%e best freuencies for operation.
,O>- SGEE6 GE>E@
est *reuencies Efficienc& (7out!
1stest f1@ IIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIII
2nd
est f2@ IIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIII
3rdest f3@ IIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIII
o# measure t%e narro# band transducerQs response not using t%e m&D/ but rat%er t%elabQs digital signal generator and 6e$troni scope. ,e do t%is because t%e ultra'sonic
transducer operates above t%e freuenc& t%e m&D/ ode instrument can %andle.
Pea$ *reuenc& IIIIIIIIIIIIIIIIIIIIII
and ,idt% IIIIIIIIIIIIIIIIIIIIII
O6E@ t%e pea$ response occurs at about 2A -G;.
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5sing t%e best freuenc& for t%e broadband spea$ers measure t%e signal strengt% vs.
#aveguide lengt%.
,O>- SGEE6 GE>E@
Signal 8evel (7olts! Pipe 8engt%
Meter IIIIIIII
12Meter IIIIIIII
1 Meter IIIIIIIII
Plot t%e signal vs. distance (lengt%!
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0
5sing t%e ultrasonic (narro# band! transducer measure t%e loss vs. distance (operate at
t%e pea$ freuenc&!.
*reuenc&@ IIIIIIIIIII
,O>- SGEE6 GE>E@
Signal 8evel (7olts! Pipe 8engt%
Meter IIIIIIII
12Meter IIIIIIII
1 Meter IIIIIIIII
Plot t%e signal vs. distance.
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1
)ontinuing to use t%e ultra'transducers measure t%e effects of bending t%e pipe b&
inserting a :0j bend.
,O>- SGEE6 GE>E@
6%roug% aW Signal Strengt%
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0ee1 : Introduction to Pro9ects "Continued#
('toElectronic Pro9ects
"n t%ese eperiments #e #ill investigate t%e use of a p%oto'source (8ED! and a p%oto
detector (p%otoconductor p%otodiode and p%ototransistor! as a position detector or as a
communications lin$.
/s a position detector t%e 8ED is ecited b& t%e continuous current in t%e circuit belo#@
*"+5>E 3. 8ED D>"7E> )">)5"6
*or communication t%e 8ED is energi;ed as in t%e circuit belo#@
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*"+5>E 3:. 8ED /) D>"7E> )">)5"6
6%e 8ED output is detected b& t%e circuit belo#@
*"+5>E )">)5"6
6%e figure belo# s%o#s a t&pical eperimental setup. ote t%e polarit& of t%e
p%otoconductor is not important %o#ever t%e p%otodiode s%ould be reverse biased i.e.
cat%ode to L and t%e p%ototransistor collector to L volts.
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/D PGO6O D"ODE >E)E"7E>
6%ree different detector devices are available@
1. P%otoconductor N t%e simplest of t%e devices but slo# in its results[2. P%otodiode N fast and reasonabl& sensitive[3. P%ototransistor N medium speed but ver& sensitive.
E;'eri)ent
)onnect t%e 8ED to t%e po#er suppl& and using a 1- o%m resistor set t%e voltage to
10 volts. 5sing t%e p%otodiode connect it as &our detector using t%e follo#ing circuit as
s%o#n@
*"+5>E
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o%m resistor #it% a DMM. Place an obstacle bet#een t%e 8ED and t%e p%otodiode and
measure t%e voltage again. ote t%e results on t%e #or$s%eet.
,O>- SGEE6 GE>E@ >esistor si;e KIIIIIIIIIIIIIIII
7oltage #it% O obstacle@ IIIIIIIIIIIIIIIIIIIIII
7oltage #it% obstacle@ IIIIIIIIIIIIIIIIIIIIII
Suc% a c%ange could be used to note t%e presence of an obstruction. 6%is is in fact #%at is
used to stop garage doors from closing #%en somet%ing is in t%e #a& or supermar$et
c%ec$out stand conve&or belts. >eplace t%e p%otoconductor #it% a p%otodiode orp%ototransistor and repeat &our measurements. O6E@ it ma& be necessar& to replace t%e
10 - o%m resistor #it% a 1 - o%m resistor due to t%e increased sensitivit& of t%ese p%oto
devices.
,O>- SGEE6 GE>E@ >esistor si;e K IIIIIIIIIIIIIII
7oltage #it% O obstacle@ IIIIIIIIIIIIIIIIIIIIII
7oltage #it% obstacle@ IIIIIIIIIIIIIIIIIIIIII
6o demonstrate communications applications #e s%all connect t%e 8ED to a function
generator and our detector circuit using a p%otodiode connected to t%e oscilloscope. See
t%e follo#ing figure.
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=
*"+5>E
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?our detector output c%annel 1 s%ould be a suare #ave. Dra# t%e output noting t%e
timescale and amplitude.
,%at %appens #%en &ou graduall& reduce t%e function generator voltage`
,%& does t%e signal suddenl& go a#a&`
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)%ange t%e function generator output to sine #aves. ,it% t%e function generator set to 10
volts amplitude dra# &our output #aveform. e sure to note amplitude and time.
o# use t%e offset adCustment of t%e function generator. Move it bot% positivel& and
negativel&. ote &our results@
)an &ou eplain #%at %appened`
IIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIII
IIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIII
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:
?ou #ill be provided #it% a P Darlington transistor #%ic% can be used in conCunction
#it% &our p%oto devices to control large loads. ?our p%oto detectors can control small
values of current i.e. micro'amperes of current to a fe# milliamperes. ?our transistor #illamplif& t%ese currents b& a factor of 1000. /ssuming t%e emitter of t%e transistor is
grounded and a current " flo#s in to t%e base of t%e transistor t%en if t%e collector is
biased %as a voltage positive #it% respect to ground t%en a collector current 1000 times
larger #ill flo#. 6%is #ill allo# &our p%oto device to control a large device suc% as t%e
motor.
See data s%eets in /ppendi D Darlington 6ransistor4.
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:0
Acoustic De+ices Pro9ects
,e s%all measure t%e free space transmission of t%e ultrasonic devices. ?ou ma& conduct
eperiments as outlined belo# or ma$e use of t%e plastic parabolic reflectors. )onnect t%e
scope c%annel 2 to t%e sine output of t%e function generator. )onnect t%e signal out to t%e
narro# band transducer. 6%e second transducer receiver s%ould be connected to c%annel
1. Eac% transducer is connected to a s%ort piece of pipe as s%o#n belo#@
*"+5>E
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:1
,O>- SGEE6 GE>E@
Distance (inc%es! Signal (volts N pea$ to pea$!
IIII04 IIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIII
IIII14 IIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIII
IIII24 IIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIII
IIII34 IIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIII
IIII
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:2
Plot &our results belo#@
Go# does t%e intensit& c%ange #it% distance i.e. rn`
IIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIII
Measure t%e angular pattern of &our transducer b& placing t%e t#o pipe ends about A4apart. Starting #it% t%e ends aligned measure t%e output as a function of lateral
displacement. See t%e figure belo#.
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:3
*"+5>E - SGEE6 GE>E@
Displacement (inc%es! Signal (volts N pea$ to pea$!
IIII04 IIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIII
IIII14 IIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIII
IIII24 IIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIII
IIII34 IIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIII
IIII
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: D>"7E )">)5"6
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0ee1 2= Pro9ect De)onstration (ral and 0ritten .e'orts
On t%e last da& of t%e laborator& eac% student (or student group! #ill be reuired todeliver a proCect verbal and #ritten report. 6%e details of t%e reporting reuirements #ill
be given to &ou b& t%e At%#ee$ b& t%e 6eac%ing /ssistant.
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/'2
I0U1( A2$ IS3LA4 S5&6I%0
7ISSI3A'I&% LI!I'I%0 1(SIS'&18 9%&:
"t is good practice to reduce t%e voltage b& setting t%e nob (*igure /2! to ;ero #%en eit%er
starting tests or c%anging polarit&. 6%e polarit& selector labeled P (positive! or PP
(negative! applies eit%er positive or negative voltage on t%e collector terminal #it% respect
to t%e emitter terminal.
6%e resistor value is c%osen to limit t%e po#er. *or eample if 1- o%m is c%osen t%en no
more t%an 20 milliamperes can flo# and t%e maimum po#er dissipation possible in t%e
device occurs if %alf of t%e voltage 2072 is across t%e device and %alf across t%e series
limiting resistor. 6%erefore 10 m/ #ould flo# and t%e po#er dissipation 10 m/ 10 7 K
100 milli#atts.
et #e need to set t%e displa& current and voltage range.
In addition, please select the . ; 2. volt range only$ o %ot operate in . ; 2.. +
#ode Serious shocks can occur if the . ; 2.. + range is used$ & %&' US( I'
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/'3
I0U1( A*$ +(1'ICAL A% 5&1I
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/'$ SU00(S'( S(''I%0S
&1 5I05 :1I05'%(SS L(S A% 5I05 3&6(1( L(S
L(') 5I05 :1I05'%(SS L( 1I05') 5I05 3&6(1( L(
)urve 6racer settings for@
Gig% brig%tness 8EDs
Series resistor (A - o%ms!
7ertical sensitivit& (1 milliamperedivision!
Gori;ontal sensitivit& (1 7division!
Gig% po#ered suare 8EDs
Series resistor (A00 o%ms!7ertical sensitivit& (10 milliamperesdivision!
Gori;ontal sensitivit& (1 7division!
Solar cells (h7
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/'A
P%otodiodes (detectors! i.e. small signal devices
Series resistor (10 - o%ms!
7ertical sensitivit& (0.2 milliamperesdivision!Gori;ontal sensitivit& (0.1 7division!
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'1
APPENDI> - Analo! MultiMeters
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'2
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'3
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'
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'A
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'=
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)'1
APPENDI> C Di!ital MultiMeters
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)'2
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)'3
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)'
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)'A
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D'1
APPENDI> D Darlin!ton Transistor
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D'2
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D'3
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