001 Lab Manual

Embed Size (px)

Citation preview

  • 7/31/2019 001 Lab Manual

    1/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    Resistors

    Objectives

    (1) To become familiar with the resistor color code and the use of

    the digital multimeter (DMM) as an ohmmeter.

    (2) To become familiar with a variable resistor (potentiometer).

    (3) To determine how the resistance of a thermistor varies with

    temperature.

    Components needed:

    Assorted 4-band and 5-band resistors Digital Multimeter

    Potentiometer Thermistor

    The Resistor

    The resistor is the most common component in electronics. A

    resistor is a two-terminal electrical or electronic component that

    opposes an electric current by producing a voltage drop between its

    terminals in proportion to the current. Resistors measure resistance, the

    ratio of the degree to which an object opposes an electric current

    through it. Resistance is measured in units called ohms () to honor

    Georg Simon Ohm (1787-1854), a German physicist credited for

    formulating the current-voltage relationship for a resistor (V = IR, Ohms

    1

  • 7/31/2019 001 Lab Manual

    2/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    Law). According to Ohms Law, the resistance R is equals to the voltage

    drop V across the resistor divided by the current I through the resistor.

    The symbols for fixed resistors and variable resistors are shown

    respectively, followed by a picture of an actual resistor showing the

    color code (Figure 1):

    Figure 1. Resistor symbols and color code.

    Fixed resistors usually come in two types: the 4-band resistor and

    the 5-band resistor. The primary difference the two is the number of

    color bands appearing in them. Both types, a resistor color code is used

    to identify the nominal values of the resistance.

    For 4-band resistors, the resistor color code is given in Table 1 below.

    Table 1. 4 Band Resistor color code

    Color1st color

    band (firstdigit - a)

    2nd color band(second digit - b)

    3rd colorband

    (exponent - c)

    4th color band(tolerance - d)

    Black 0 0 0Brown 1 1 1 1%

    Red 2 2 2 2%Orange 3 3 3 3%Yellow 4 4 4 4%Green 5 5 5Blue 6 6 6Violet 7 7 7Gray 8 8 8White 9 9 9

    2

  • 7/31/2019 001 Lab Manual

    3/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    Gold -1 5%Silver -2 10%

    No color 20%

    The resistor color code is used to identify the nominal values of the

    resistance as follows:

    4-Band Resistors: The first two colored bands (a & b, closest to

    the end of the resistor in Figure 1) determine the first two digits

    of the resistor value. Table 1 shows the listing of the numerical

    value associated with each color. The third band (c) determines

    the exponent of the power-of-10 multiplier i.e. the number of

    zeros following the first 2 digits. The fourth band (d)

    determines the tolerance of the resistor.

    Resistance = (10a + b) x 10c d

    For example, a 21 kiloohm 5% resistor has the color bands red,brown, red, and gold. Common prefixes used for resistors arekilo(k) and mega (M).

    For 5-band resistors, the resistor color code is given in Table 1 below.

    Table 2. 5-Band Resistor Color Code

    Color 1st colorband, firstdigit (a)

    2nd colorband,seconddigit (b)

    3rd colorband,thirddigit (c)

    4th colorband,exponent(d)

    5th colorband,tolerance(e)

    Black 0 0 0 0Brow 1 1 1 1 1%Red 2 2 2 2 2%

    Orange 3 3 3 3 3%Yellow 4 4 4 4 4%Green 5 5 5 5Blue 6 6 6 6Violet 7 7 7 7Gray 8 8 8 8White 9 9 9 9Gold -1 5%

    3

  • 7/31/2019 001 Lab Manual

    4/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    Silver -2 10%No Color 20%

    5-Band Resistors: The first three colored bands (a, b, and c,

    first three of the four adjacent color bands), determine the firstthree digits of the resistor value. The fourth band (d)

    determines the exponent of the power-of-10 multiplier, i.e., the

    number of zeros following the first two digits. The fifth band (e),

    the color band farthest from the four adjacent color bands,

    determines the tolerance of the resistor. Thus,

    Resistance = (100a + 10b + c) x 10d e

    For example, an 82.5 kiloohm 1% resistor has the color bands gray,

    red, green, red, and brown.

    4

  • 7/31/2019 001 Lab Manual

    5/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    Measuring Technique

    Resistance is never measured in a live circuit using a DMM because the resistor

    might be damaged. The resistor to be measured should be removed from the circuit to

    ensure that your measurement will not be affected by any other components of the circuit.

    Make sure also that when you measure the resistor, only the probes of the DMM are

    touching the resistor. In other words, avoid touching the resistor as much as possible.

    There is no calibration for the DMM. Short (connect) the leads together and the

    DMM should display zeros (or less than 0.3 ohms). Any resistance above the maximum for

    a selected scale will result in the display showing 1 or OL or sometimes constantly

    fluctuating. Adjust the DMM to the correct scale.

    Exercise

    A.Nominal vs. Actual Resistance

    Get five different resistors from your instructor. Record the nominal resistance of

    the resistors (based on Tables 1 or 2, depending on the number of color bands), the actual

    resistance (based on the DMM reading), and the percent discrepancy between the nominal

    and actual resistance readings of each resistor. Calculate for the minimum and maximum

    tolerance resistance by subtracting or adding a specific amount based on the tolerance of

    the resistor. Actual Tolerance is difference of actual from nominal resistance.

    Ex: For a 12 kiloohm 5% resistor (brown, red, orange, gold color code) has a

    maximum tolerance resistance of [12,000 + (12,000 *.05)] kiloohm = 12.6 kiloohm. It has

    a minimum tolerance of [12,000 - (12,000 *.05)] kiloohm = 11.4 kiloohm.

    5

  • 7/31/2019 001 Lab Manual

    6/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    Compute % Discrepancy as:

    B. Potentiometer

    Get a variable resistor / potentiometer from your instructor. The resistance of the

    potentiometer varies by twisting its knob. Determine the maximum and minimum

    resistance values of your potentiometer by twisting the knob to the left and right.

    To measure, attach the middle wire of the potentiometer to the ground probe (black)

    of the DMM. After this, attach either left or right wire of the potentiometer to the positive

    probe (red) of the DMM. Refer to Figure 2 below:

    Figure 2: How to Measure Resistance from the Potentiometer

    6

  • 7/31/2019 001 Lab Manual

    7/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    C. Thermistor

    Get a thermistor from your instructor. The resistance of the thermistor varies with

    respect to temperature.

    First, get the resistance of the thermistor in an air-conditioned room. Record the

    resistance reading as Raircon. Measure the temperature of the room and record it as Taircon.

    Second, clamp the thermistor tightly between two fingers. Get the resistance of the

    thermistor after 5 to 10 minutes. Record the resistance reading as Rbody. Clamp the

    thermometer between your fingers and measure the temperature and record it as Tbody.

    Lastly, get the resistance of the thermistor outside of the air-conditioned room.

    Equilibrate for at least 10 minutes. Record the resistance reading as Routside. Measure the

    temperature outside the room and record it as Toutside.

    Using the obtained Raircon, Rbody, Taircon, and Tbody, construct a two-point calibration

    curve using MS Excel or linear regression from a scientific calculator. From the recorded

    Routside, solve for Toutside, theoretical using the equation derived from the calibration curve.

    Compare the computed value to the recorded Toutside and solve for the %difference:

    Obtain the slope of the line to solve forR/T which has units of (/C)

    Sources:

    (1) Oppus, C.M. PS 141 Laboratory Manual. 2nd ed, 2003.

    (2) Malmstadt, H.V.; Enke, C.G.; Crouch, S.R. Laboratory Electronics for

    Scientists, 2nd Ed., 1994.

    7

  • 7/31/2019 001 Lab Manual

    8/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    Resistors

    Group Name: ________________________ Section: ________

    Name: ______________________________

    Raw Data Tables:Resistor Color Code Nominal R % Tolerance

    1

    2

    3

    4

    5

    Derived Data Tables:

    Resistor

    Actual

    Tolerance

    R

    Min.

    Tolerance RMax. Tolerance R Actual R

    %

    Discrepancy

    1

    2

    3

    4

    5

    8

  • 7/31/2019 001 Lab Manual

    9/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    B.

    Maximum Resistance of Potentiometer: ____________________

    Minimum Resistance of Potentiometer: ____________________

    C.

    Resistance Temperature

    Air-conditioned room

    Body

    Toutside, theoretical: ______ Toutside, derived:______ %difference: __________

    Routside: ____________R/T = _________

    9

  • 7/31/2019 001 Lab Manual

    10/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    1. Why is it necessary that only the probes of the DMM are touching the resistor?

    2. How does the thermistor resistance change with temperature? How would you

    describe its temperature coefficient?

    3. (For out-of-classroom research) How is a potentiometer constructed? What are the

    three terminals of the potentiometer for?

    10

  • 7/31/2019 001 Lab Manual

    11/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    The Breadboard

    Objectives

    (1) To become familiar with the uses of a breadboard.

    (2) To determine the connection arrangement of a breadboard.

    Components needed:

    Breadboard Digital Multimeter

    The Breadboard

    The breadboard is used to create a circuit without the need for

    soldering circuit elements together. The upper and lower halves of the

    breadboard contain 64 vertical rows of 5 interconnected contacts. There

    are also 4 long horizontal rows of connectors (5 groups of 5 contacts

    each) along the upper and lower edges. These long rows of connectors

    are referred to as power bus strips because they will be connected to

    the power supplies to provide power connections over the entirety of the

    breadboard. This breadboard socket is designed to accept integrated

    circuits, most common wire terminal components, and wire

    interconnections.

    11

  • 7/31/2019 001 Lab Manual

    12/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    Exercise

    Switch the DMM to measure resistance (any scale will do). Again,

    keep in mind that a short circuit gives a reading of 0 while an open

    circuit gives a reading of infinite resistance (1 or 0L).

    Insert wires into the breadboard holes carefully. Grasp the wire

    with your hands about inch from the end to be inserted and push into

    the breadboard until it is firmly in place.

    Figure 1. The Breadboard.

    Use the DMM to confirm the connection arrangement of the breadboard.

    Draw the verified connection arrangement of the breadboard given to

    you in the space below.

    12

  • 7/31/2019 001 Lab Manual

    13/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    Source:

    (1) Malmstadt, H.V.; Enke, C.G.; Crouch, S.R. Laboratory Electronics

    for Scientists 2nd Ed. 1994.

    13

  • 7/31/2019 001 Lab Manual

    14/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    Power Supply

    Objectives

    (1) To connect a regulated power supply to the breadboard.

    (2) To differentiate between regulated and unregulated power

    supplies.

    Components needed:

    Breadboard Digital Multimeter

    Power Sockets (2)

    Jumper wires 100 1-W resistors (2)

    0.1 uF ceramic capacitor

    1 uF tantalum capacitor 2.2 or 3.3 uf tantalum or electrolytic capacitors

    Voltage regulators (7805 and 7905)

    Exercise

    A. Unregulated Power Supply

    Install the two power supply sockets into the breadboard as shown

    below (Figure 1). Also attach the wires as shown in the diagram. The

    wire colors are not necessary; they are just a useful reminder of what

    each line is carrying (red = positive, yellow = negative, black =

    ground/common).

    14

  • 7/31/2019 001 Lab Manual

    15/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    Figure 1. Installing the power supply sockets.

    Plug one adapter into one of the sockets. Using the DMM, measure

    the voltage between the red and black power buses. This should be

    around 9-12 V. This is the DC output voltage without load. Keep in mind

    however that the DMM has an internal 10 M resistance.

    An unregulated power supply will have a fluctuating output

    voltage depending on the load connected to it.

    Connect two 100 1-W resistors in series. Connect one end to the

    power supply and the other end to ground. Again, measure the output

    voltage.

    Disconnect the power supply. Are the resistors hot?

    B. Creating a Regulated Power Supply

    15

  • 7/31/2019 001 Lab Manual

    16/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    Figure 2. Schematic diagram for the regulated power

    supply.

    To regulate the voltage output of the unregulated power source, one

    uses a full-wave rectifier-filter circuit, as shown in Figure 2. In your

    breadboard, add the circuit elements as shown in Figures 3 and 4. Make

    sure that you follow the polarities of the capacitors. The longer wire of

    the capacitor is the positive end. The capacitors are added to prevent

    noise and oscillation and to increase the stability of the output voltage.

    C

    Figure 3 Figure 4

    16

  • 7/31/2019 001 Lab Manual

    17/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    Connect the voltmeter across the red and black power buses. Plug

    the power supply to the positive power socket. Disconnect immediately

    if the voltage is not within 5% of +5 V or if the regulator becomes hot.

    Record the positive regulated voltage without load.

    Now connect the voltmeter across the yellow and black power

    buses. Plug the power supply to the negative power socket. Disconnect

    immediately if the voltage is not within 5% of 5 V or if the regulator

    becomes hot. Record the negative regulated voltage without load.

    Connect two 100 1-W resistors in series. Connect one end to the

    positive regulated power supply and the other end to ground. Measure

    the output voltage with load. Compare this to the data you got earlier.

    The regulators will become hot so do not keep the connections for long

    periods.

    17

  • 7/31/2019 001 Lab Manual

    18/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    Source:

    (1) Malmstadt, H.V.; Enke, C.G.; Crouch, S.R. Laboratory Electronics

    for Scientists 2nd Ed. 1994.

    18

  • 7/31/2019 001 Lab Manual

    19/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    Power Supply

    Group Name: _________________

    Name: ______________________________

    A.

    Unregulated voltage output without load: __________

    Unregulated voltage output with load: __________

    B.

    Regulated voltage output without load: __________

    Regulated voltage output with load: __________

    1. What is the purpose of regulating the power supply?

    2. Explain briefly the process of converting the 220 V AC power

    supply to the 5 V DC regulated power supply.

    19

  • 7/31/2019 001 Lab Manual

    20/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    Resistors in Series and Parallel

    Objective

    To become familiar with the different resistive connections

    particularly parallel and series connections.

    Components needed:

    Regulated Power Supply from Experiment 3 Digital Multimeter

    Assorted Resistors (3)

    Series and Parallel

    Series resistor configuration consists of two or more resistors

    connected tail to head with the open terminals as the series connection

    terminals as shown below (Fig. 1):

    Figure 1. Resistors in series.

    The effective resistance of resistors in series is equal to the sum of

    their individual resistances:

    =

    =n

    i

    iequiv RR1

    Equation 1

    20

  • 7/31/2019 001 Lab Manual

    21/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    Parallel resistor configuration consists of two or more resistors

    connected tail to tail then head to head with the head connection

    forming one of the terminals and the tail connection forming the other,

    as shown below (Figure 2):

    Figure 2. Resistors in parallel.

    The inverse of the effective resistance of parallel resistors is equal

    to the sum of the inverses of their individual resistances:

    Exercises

    Part A.

    Get 3 different resistors from your instructor. With the concepts of

    series and parallel circuits in mind, construct a circuit with your 3

    resistors such that the minimum resistance value is obtained. Connect

    this new resistor to the 5-V regulated power source (with the other

    end connected to ground).

    =

    =n

    i iequivRR 1

    11 Equation

    21

  • 7/31/2019 001 Lab Manual

    22/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    Also, connect the multimeter in series with the new resistor. Get

    the value of the current, I (make sure that the DMM is properly

    configured). Using Ohms law (V = IR), youll be able to get the

    experimental R. Using the appropriate equation, youll be able to get the

    nominal R. Determine the % difference of the two values.

    Disconnect the multimeter from the circuit but keep the circuit intact.

    Read the voltage across each resistor by connecting the DMM in parallel

    across each one (make sure that the DMM is properly configured). Also,

    read the current flowing through each resistor by connecting the DMM in

    series to each (again, make sure that the DMM is properly configured).

    Part B.

    Using the resistors you used earlier, construct a circuit such that the

    maximum resistance is obtained. Connect this new resistor to the 5-V

    regulated power source.

    Connect the multimeter in series with this new resistor. Get the

    value of I. With this value, get the experimental value of R. Compare this

    with the nominal value of R of your circuit. Determine the % difference

    of the two values.

    Disconnect the multimeter from the circuit but keep the circuit intact.

    Get the current through each resistor and the voltage across each

    resistor using the DMM.

    22

  • 7/31/2019 001 Lab Manual

    23/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    Source:

    (1) Oppus, C.M. PS 141 Laboratory Manual. 2nd

    Ed, 2003.

    23

  • 7/31/2019 001 Lab Manual

    24/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    Resistors in Series and ParallelGroup Name: _________________Name: _______________________________

    A. Icicruit:____________

    Rnominal :___________ Rexpt:_____________ %

    difference_____________

    Vequivalent:__________

    Resistor Resitance/ Voltage (V) Current (I)

    Nomin

    al

    Actua

    l

    Calculate

    d Actual

    Calculat

    ed

    Actua

    l

    Calculat

    edR1

    R2

    R3

    Total

    B. Icicruit:____________

    Rnominal :___________ Rexpt:_____________ %

    difference_____________

    Vequivalent:__________

    Resistor Resitance/ Voltage (V) Current (I)

    Nomin

    al

    Actua

    l

    Calculate

    d

    Actual Calcula

    ted

    Actua

    l

    Calculat

    edR1

    R2

    R3

    Total

    24

  • 7/31/2019 001 Lab Manual

    25/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    1. What do you observe about the voltage across each resistor in A?

    Add up all current values through each resistor. How is this related

    to I of the whole circuit?

    2. What do you observe about the current through each resistor in B?

    Add up all the voltages of each resistor. How is this related to the

    V of the whole circuit?

    25

  • 7/31/2019 001 Lab Manual

    26/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    3. Why is there a discrepancy between the nominal and experimental

    values of resistances?

    26

  • 7/31/2019 001 Lab Manual

    27/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    Diodes

    Objective

    To become familiar with the uses of a diode.

    Light-emitting diode

    A diode is a device which allows the flow of current in a circuit in a

    single direction. Ideally, the diode is just a conductor, i.e., it has zero

    resistance. The circuit symbol of a light-emitting diode is shown below

    (Figure 1):

    Figure 1. Circuit symbol of a light-emitting diode.

    A light-emitting diode (LED) follows that same principle. However,

    it utilizes the current that passes through it to give off light.

    Exercise

    Part A

    Construct the circuit shown in Figure 2. You may use wires to

    make the switch, just connect or disconnect the wires as necessary.

    Check your circuit by turning on the switch and checking the current on

    the end of the diode connected to ground. If there is no current, invert

    the position of your diode.

    27

  • 7/31/2019 001 Lab Manual

    28/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    Figure 2. Diode circuit.

    What is the current? Is this the current that you expected with the

    220 resistor?

    Part B

    Replace the diode with a light-emitting diode. If no light is emitted

    by the LED, invert its position. Add more LEDs in series and in parallel

    to the original LED in the circuit. What happens to the intensity of the

    light of the LEDs?

    Part C

    Again, construct the circuit shown in Figure 1, but this time,

    replace the resistor with a potentiometer and the diode with an LED.

    Make sure you connect the potentiometer correctly, i.e., the resistance

    varies as the knob is turned. Turn on the switch. What happens to the

    intensity of the light of the LED when you turn the knob?

    28

  • 7/31/2019 001 Lab Manual

    29/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    Sources:

    (1) http://stage.itp.nyu.edu/~tigoe/pcomp/labs/assign1.shtml

    accessed March, 2003.

    (2) Horowitz, P.; Hill, W.; The Art of Electronics. 2nd Ed. Cambridge

    University Press, 1991.

    Diodes

    Group Name: _________________

    Name: ______________________________

    A.

    Theoretical current : __________

    Actual current: __________

    Diode resistance: __________

    1. How does adding more resistors and LEDs to the circuit affect the

    intensity of the light? Does it matter whether the LEDs are

    connected in series or in parallel?

    29

    http://stage.itp.nyu.edu/~tigoe/pcomp/labs/assign1.shtmlhttp://stage.itp.nyu.edu/~tigoe/pcomp/labs/assign1.shtmlhttp://stage.itp.nyu.edu/~tigoe/pcomp/labs/assign1.shtml
  • 7/31/2019 001 Lab Manual

    30/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    2. How does resistance in series to the LED affect the intensity of the

    light?

    30

  • 7/31/2019 001 Lab Manual

    31/115

    Figure 1. The operational amplifier terminal diagram.

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    Operational Amplifiers

    Objective

    To become familiar with the different configurations of an

    operational amplifier.

    Materials

    +5V/-5V power supply from Experiment 3

    LF353 operational amplifier

    1 or 2.5k potentiometer

    Two 2.2k resistors

    One 10k resistor

    One 47k resistor

    One 22k resistor

    Digital multimeter

    Two DC converters

    Green or yellow LED

    Dark cover for LED

    Operational amplifier

    The terminal diagram of an operational amplifier is shown below

    (Figure 1).

    31

  • 7/31/2019 001 Lab Manual

    32/115

    Figure 2. LF353 op-amp pin configuration

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    The operational amplifier amplifies the voltage across its two

    inputs by a gain factor. The gain to which the input voltage difference is

    amplified depends on the values of the feedback elements.

    The operational amplifier that you will use for this exercise is the

    LF353. The pin configurations are shown in Figure 2.

    Exercise

    A. Inverting amplifier

    Construct the variable-voltage source using a 1 or 2.5k

    potentiometer placed between two 2.2k resistors. One end of both

    32

  • 7/31/2019 001 Lab Manual

    33/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    resistors are then connected to the +5V/-5V power supply from

    Experiment 3 as shown in Figure 3.

    Figure 3. Op-amp Inverting Amplifier

    Test that the variable voltage source can go from -1 to +1V as the

    potentiometer knob is turned. This can be done by using a digital

    multimeter. Connect one probe of the multimeter on the center terminal

    of the potentiometer and the other one will be on one end of the

    potentiometer.

    The variable-voltage source will serve as the input for the op-amp

    inverting amplifier. This will also be the voltage input, Vin, which will be

    recorded.

    On the breadboard, insert the op-amp integrated circuit (IC)across the center channel as shown in Figure 4. Consult Figure 3 to

    construct the remaining parts of the circuit.

    33

  • 7/31/2019 001 Lab Manual

    34/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    Figure 4. Placing the op-amp onto the breadboard.

    Vary Vin by turning the potentiometer knob from the maximum

    allowable voltage to approximately 0.50V, 0.25V, 0.00V, -0.25V, -0.50V,

    and the minimum allowable voltage. Record the voltage output, Vout,

    together with the actual Vin. Vout can be acquired from the digital

    multimeter readout.

    B. LED as a light detector

    Use an LED as a light detector together with an op-amp current-to-

    voltage converter. Normally, an LED is used to emit light when current is

    passed through it. However, when the LED is illuminated, it creates a

    small current and can be used as a photodiode light detector.

    Construct the circuit shown in Figure 5. Use only a yellow (preferred)

    or a green LED. Do not use a red LED. You need to use only one op-amp

    in the IC. NOTE: You must ensure that the LED is reverse-based. If the

    LED lights up, reverse it.

    34

  • 7/31/2019 001 Lab Manual

    35/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    Figure 5. LED circuit diagram.

    With the LED covered, measure the voltage output. Remove the

    cover of the LED, exposing it to light. Again, measure the voltage output

    of the operational amplifier.

    Use an LED as a light detector together with an op-amp current-to-

    voltage converter. Normally, an LED is used to emit light when current is

    passed through it. However, when the LED is illuminated, it creates a

    small current and can be used as a photodiode light detector.

    35

  • 7/31/2019 001 Lab Manual

    36/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    Source:

    (1) Malmstadt H.V.; Enke, C.G.; Crouch, S.R. Laboratory Electronics

    for Scientists 2nd

    Ed. 1994.

    36

  • 7/31/2019 001 Lab Manual

    37/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    Operational Amplifiers

    Group Name: _________________ Name:

    ______________________________

    Part 1.

    R1 (input): ____________ ohms R2 (feedback resistor):

    ___________ohms

    Vin

    (nominal)

    Vin

    (expt.)

    Vout

    (theoret.)

    Vout

    (expt.)

    Gain (Vout / Vin)

    -1.00-0.50-0.250.000.250.501.00

    1. What is the value of gain and how does it relate to the values of R1

    and R2?

    2. The gain decreases as the op-amp output voltage approaches the

    supply voltages. This is called saturation. What is the

    approximate positive saturation voltage?__________ Negative

    saturation voltage? ________________.

    37

  • 7/31/2019 001 Lab Manual

    38/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    Part 2.

    Compute the current through the LED by dividing the voltage output by

    the value of the resistor used. The voltages are in the milli-volts and

    may fluctuate, so just use the average.

    Range of V output with covered LED: __________ mV Current:

    ____________

    Range of V output with uncovered LED: _________ mV Current:

    ____________

    1. The circuit you designed has the basis for photodetection, with the

    LED as a primitive detector. Which instruments find use for a

    photo-detector?

    2. Was the output steady? Noise is a major issue in signal

    amplification. How come

    38

  • 7/31/2019 001 Lab Manual

    39/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    39

  • 7/31/2019 001 Lab Manual

    40/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    RC Filters

    Objective

    To introduce students to the different types of filters, specifically the RC

    filter circuit.

    RC Circuit

    A capacitor can store an electric charge while a resistor dissipates the

    flow of charges as heat. A fully charged capacitor, when connected across a

    resistive element, will lose its charge as current flows across the resistor.

    Connecting a voltage source across a series R-C circuit will cause a charging

    current to flow. This current changes with time as the voltages across the

    resistor and capacitor changes.

    By changing the source to a sine source, the frequency dependent

    voltage and current relationship in a capacitor can be exploited. The capacitor

    has a frequency-dependent resistance referred to as capacitive reactance.

    By combining resistors and capacitors in RC circuits, a frequency-dependent

    voltage divider circuit is realized. Thus is created a circuit in which the input

    and output relationships are frequency-dependent. These circuits form the

    basis of filters.

    Filters

    Fundamentally, all periodic fluctuations can be by a reduced to

    combination of sine waves of different frequencies. Electrical signals are no

    exception, and thus have their signature frequencies. In most cases, the

    40

  • 7/31/2019 001 Lab Manual

    41/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    frequency of the desired signal is known. Stray signals of different frequencies,

    or noise, interfere with the transmission of signals. Most of the time, these

    stray signals are unavoidably combined with the desired signal. However,

    there are ways to remove the noise from signal transmissions.

    Filters are used to weed out the unwanted signal frequencies. There are

    four basic types of filters. A low-pass filter only lets lower frequencies pass

    through. A high-pass filter lets higher frequencies pass through. A band-select

    filter only lets a certain range of frequencies to pass through. A band-reject

    filter lets all frequencies pass through except for a certain range of

    frequencies.

    In this lab, a simple RC filters characteristics are demonstrated.

    Exercise

    Filter Circuit

    Construct the filter circuit shown below using CircuitMaker. The devices

    and elements to be used can be found under .General in the Major

    Device Class.

    41

  • 7/31/2019 001 Lab Manual

    42/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    Figure 1 RC filter circuit

    Access the Device Selection window (Figure 2) by clickingDevices>Browse

    Figure 2 Device Selection window with listed devices

    42

  • 7/31/2019 001 Lab Manual

    43/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    Under Major Device Class, select and place the following circuit

    components in your circuit setup

    Circuit

    Component

    Directory

    SignalGenerator

    .General>Instruments>SignalGenerator

    Multimeter .General>Instruments>Multimeter

    Resistor .General>Resistors>Resistor

    Capacitor .General>Capacitors>Capacitor

    Ground .General>Sources>Ground

    Set parameters of the devices and elements in the experiment bydouble-clicking on devices and making the following changes to

    the device parameters:

    CircuitComponent

    New Parameter

    Signal Generator Peak amplitude =1.41 VFrequency = 1.000kHz

    Multimeters Measure AC RMSResistor Resistance = 10k

    ohms

    Capacitor Capacitance = 0.1 uF

    Figure 3 (Right)

    Editing parameters of the

    signal generator

    43

  • 7/31/2019 001 Lab Manual

    44/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    Click on the Running Man icon to run the analysis. Theoscilloscope window should appear and the cursor should becomea probe.

    Select the voltage input and output nodes by holding the SHIFT key

    and selecting the areas highlighted in Figure 4. If done correctly,

    then waves similar to those in Figure 5 will appear on the

    oscilloscope window.

    Figure 3 Select the highlighted areas to measure voltage input and output

    using the probe tool.

    Figure 5 Waves generated in the oscilloscope window. Plotmarkers measure the phase shift at the amplitude of eachwave

    44

  • 7/31/2019 001 Lab Manual

    45/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    Measure the phase shift between output and input by dragging plot

    markers a and b to the amplitudes of each wave (as shown in

    Figure 4). Measure the amplitudes by dragging plot markers c and

    d along the right edge of the oscilloscope. List the measurements

    in Data Table 1.

    To stop the simulation, click on the stop icon . Once the analysis

    has stopped, adjust the signal generator frequency to 100 Hz and

    measure the phase shifts and amplitudes.

    Repeat this procedure for 10 Hz, 100 Hz, 160 Hz, 1kHz and 10 kHzfrequencies. Record the data in Data Table 1.

    NOTE:

    For low-frequency setups (i.e. 100 Hz and below), open the

    Analyses Setup window by clicking Simulation>Analyses Setup.

    Click on the Transient/Fourier button. Change the Step Time to

    10.00 uS, Max Step to 10.00 uS and Stop Time to 100.00 mS.

    Confirm the changes.

    For frequencies above 1 KHz, adjust the Step Time to 1.00 uS and

    Max Step to 1.00 uS.

    Bode Plot

    Disassemble the filter circuit. Construct the new circuit as shown in

    Figure 6 below.

    45

  • 7/31/2019 001 Lab Manual

    46/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    Figure 7 New circuit setup with capacitor as test point

    Select voltage across the capacitor with the probe tool

    To set up and run an AC analysis, connect a signal generator to thecircuit. Double-click on the signal generator to open the window inFigure 8a. Click on Wave to access the window in Figure 8b. CheckSource underAC Analysis.

    Figure 8 a) Left. Edit Sine Wave window. b) Edit signal generatorwindow.

    Go to Simulation>Analyses Setup and disable all options exceptAC(as in Figure 9)

    46

  • 7/31/2019 001 Lab Manual

    47/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    Figure 9 Uncheck all options in Analyses Setup window except for AC

    In the same window, click on AC and check Enabled. Change the Start

    Frequency to 10. 00 Hz, the Stop Frequency to 10.00 kHz, the

    number of test points to 10 and then select Decade Sweep (as in

    Figure 10)

    Figure 10 AC Analysis Setup window

    Run the simulation. Open the Graph Settings window (Figure 11) by

    clicking on the Graph Settings icon . Use this window to make

    adjustments to the oscilloscope graph settings. Adjust and view

    the following graph settings in the oscillograph. Observe how the

    graphs are able to quickly perform and plot the phase shift

    measurements in Part A.

    X-grid Functio

    n

    Y-Grid Functio

    n

    47

  • 7/31/2019 001 Lab Manual

    48/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    Magnitud

    e

    Log X Magnitude Linear Y

    Magnitud

    e

    Log X Magnitude Log Y

    Magnitude

    Log X Phase indegrees

    Linear Y

    Figure 11 Graph Settings window. Parameters for the x and y-axes

    as well as the function can be changed in this window

    Swap the positions of the resistor and capacitor. Again obtain the

    amplitudes and phase shifts of the signals at 10 Hz, 100 Hz, 160

    Hz, 1kHz and 10kHz. Also obtain the Bode plots as in the previous

    number.

    48

  • 7/31/2019 001 Lab Manual

    49/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    Source:

    (1) Boylestad, R.L.; Nashelsky, L. Electronic Devices and Circuit Theory, 8th Ed., Prentice

    Hall, 2002

    (2) Modifications from Electronics Class 2009.

    49

  • 7/31/2019 001 Lab Manual

    50/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    RC Filters

    Group Name: _________________

    Name: ______________________________

    DATA

    Note: Report all data (voltage, frequency and phase shift) up to 4

    significant figures

    Table 1

    Frequenc

    y

    Vin (V) Vout (V) Vout/ Vin * t [a-b]

    (s)

    Phase

    Shift ()10 Hz100 Hz160 Hz

    1 kHz10 kHz

    *time delay between input and output waveform

    1. Compute the phase shift as follows:

    (degrees) = t x f x 360

    where f = frequency

    2. Using the data above, plot the frequency response in the graphs provided.

    What type of filter is this? _____________________

    50

  • 7/31/2019 001 Lab Manual

    51/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    51

  • 7/31/2019 001 Lab Manual

    52/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    3. Using the data above, find the frequency where Vout = 0.707Vin.

    Frequency = ___________ Hz

    Compare this with fc = 1/ (2RC) where R= resistance, C= capacitance.

    4. What is the phase shift at this frequency?

    Phase shift = ___________ degrees (indicate sign)

    5. Encircle your answer: In this circuit, Vout lags/leads Vin

    Table 2 (after swapping R and C)

    Frequenc

    y (f)

    Vin (V) Vout (V) Vout/ Vin t (a-b)

    (s)

    Phase

    Shift ()10 Hz100 Hz160 Hz1 kHz10 kHz

    6. Compute the phase shift as follows:

    (degrees) = t x f x 360

    7. Using the data above, plot the frequency response in the graphs provided.

    What type of filter is this? _____________________

    52

  • 7/31/2019 001 Lab Manual

    53/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    53

  • 7/31/2019 001 Lab Manual

    54/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    8. Using the data above, find the frequency where Vout = 0.707Vin.

    Frequency = ___________ Hz

    Compare this with fc = 1/ (2RC)

    9. What is the phase shift at this frequency?

    Phase shift = ___________ degrees (indicate sign)

    10. Encircle your answer: In this circuit, Vout lags/leads Vin

    54

  • 7/31/2019 001 Lab Manual

    55/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    Digital Electronics

    Objectives

    The experiment aims to:

    to familiarize the students with the use of TTL ICs and the truth table.

    to be able to construct circuits using the AND, OR, NAND and NOR TTL

    ICs

    to solve logic problems using the different logic gate combinations.

    Material

    7408

    7432

    7402

    7400

    Digital Multimeter (DMM) Power Supply with 5 V regulator

    Wires

    Theories and Concepts:

    Logical Operations

    Aside from arithmetic operations and binary numbers, the basis of

    digital electronics includes logical operations. The most common logic

    operations are NOT, OR and AND operations. Each logic operations are

    used differently from each and used in different logic problems.

    55

  • 7/31/2019 001 Lab Manual

    56/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    COMMON LOGIC OPERATIONS

    NOT operation

    This logic operation produces an output that is the

    compliment of the operand or the input. For example, if your input

    is equal to 1, then using the NOT operation would result to an

    output equal to 0. In some notations, stating this would be: NOT

    1=0. The symbol for NOT is - or by putting a bar above the

    operand.

    Example:

    -(10010) = 01101

    100101 = 011010

    OR operation

    This logic operation produces an output equal to 1 if there is

    at least one operand or input that is equal to 1. For example,given the inputs 1010, using the OR operation would result to an

    output equal to 1 since there is at least one operand equal to 1. In

    some notations, we could state this example as 1 OR 0 OR 1 OR 0

    = 1. The symbol for OR is +.

    Example:

    1 + 0 = 1, 0 + 0 = 0

    10001 + 01010 = 11011

    AND operation

    This logic operation produces an output that is equal to 1 if

    all the inputs are equal to 1. If at least one of the operand is equal

    56

  • 7/31/2019 001 Lab Manual

    57/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    to 0, the output will be 0. For example, given the inputs 1011,

    using the AND operation would result to an output equal to 0 since

    there is an input equal to 0 in the given (can also be stated as: 1

    AND 0 AND 1 AND 1 = 0). Given the inputs 1111, using the same

    operation would give an output reading equal to 1 since all inputs

    in the given is equal to 1 (can also be stated as: 1 AND 1 AND 1

    AND 1 = 1). The symbol for AND is &.

    Example:

    11111 & 10001 = 10001

    00000 & 11111 = 00000

    Other operations:

    The NOR and NAND operations are basically the OR and

    AND operations with their inputs negated (NOT-OR AND NOT-

    AND).

    Example:

    10100 NOR 11010 = 00001 10111 NAND00101 = 11010

    00001 NOR 10001 = 01110 11100 NAND

    10101 = 01011

    Logic Gates

    The logic gates that are used today in integrated chips (ICs) use

    transistors to simulate logical operations, thus they are called transistor-

    transistor logic (TTL) ICs. The ICs that will be used in the experiment are

    quad 2-input logic gates. The quad term refers to the number of logic

    gates in the IC and the 2-input means that each logic gates requires 2

    inputs to operate. In other words, there are four logical operating units

    in each IC taking in two separate inputs each.

    57

  • 7/31/2019 001 Lab Manual

    58/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    Logic gate operations can be used in combination with each other in

    order to produce a desired set of output values as written in your truth

    table. TTL ICs can be used with each other to make circuits with the

    desired output value.

    Examples of Possible Ways of Combining Logic Gate Operations are

    shown in Figure 2.

    Figure 2. Possible Ways of Combining Logic Gates

    Truth Tables

    The truth table is an easy way of determining how a logical

    operation proceeds given the different possibilities of inputs. In this

    table, all possible input combinations are listed. Using a specific logicoperation, the output is also tabulated at the last column of the table.

    Example: Using the AND logic gate and a 2-input system:

    Figure 3: AND Truth Table

    A B Y(output)

    0 0 00 1 0

    1 0 01 1 1

    Exercise

    A. Basic Logic Gates

    58

  • 7/31/2019 001 Lab Manual

    59/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    Each student will be provided with two of the following ICs: 7400, 7402,

    7408, and 7432. These are the AND, OR, NAND and NOR quad gates. The pin

    assignments are shown below:

    Connect the Vcc to +5 V

    and the ground pin to ground.

    Five volts applied to an input of the IC is considered a signal high (1).

    This voltage requirement is for TTL but for other low-powered ICs like CMOS,

    the voltage requirements for a signal high may be lower. Connecting the input

    to ground is considered a signal low (0). Using the DMM connected to the

    output and to the ground, construct the truth table for each of your ICs as

    shown below:

    7400 7402

    7408 7432

    59

  • 7/31/2019 001 Lab Manual

    60/115

    Electronics Laboratory for the Physical Sciences

    I.M.S. De Vera, M.J. M. Garrovillas and E.T. Chainani

    Exhaust all possible combinations of inputs and check the outputs of

    each. Any voltage read from the output of the IC is considered a signal high. A

    0-V output is a signal low.

    AND GateA B Y0 00 11 01 1

    ORA B Y

    0 00 11 01 1

    NANDA B Y0 00 11 01 1

    NORA B Y0 00 11 01 1

    60

  • 7/31/2019 001 Lab Manual

    61/115

    B. The XOR operation

    Another important logical operation is the exclusive OR or

    XOR (F = x y). This is important in applications where only a

    single high input generates an output high. The XOR truth table is

    shown below:

    Table 1. XOR Truth Table

    x y F0 0 00 1 1

    1 0 11 1 0

    Using the two ICs you have, construct an XOR circuit. Draw

    the schematic diagram of the circuit; draw the pertinent logic

    gates and show how they are connected.

    Hint: If you need to negate an input, you may use the NAND or

    NOR gates. Any signal applied to both inputs of one of those gates

    will generate the complement in the output.

    C. Application

    A certain instrument has three sensors for pressure,

    temperature, and humidity. Abnormal conditions (high

    temperature, low pressure, high humidity, etc.) cause the sensor

    to generate a signal high. The instrument is designed to continue

    operating even if abnormal pressure or humidity is detected, but

  • 7/31/2019 001 Lab Manual

    62/115

    not both at the same time. The instrument is not allowed to

    operate at abnormal temperatures.

    Construct a truth table for the sensing mechanism of this

    instrument. Using the ICs provided, construct such a mechanism.

    You may ask for additional ICs from your instructor.

    Since this is a 3 input instrument, there will be 8 possible inputcombinations (23=8).

    Truth Table for the InstrumentT P H Y0 0 0

    0 0 10 1 00 1 11 0 01 0 11 1 01 1 1

  • 7/31/2019 001 Lab Manual

    63/115

    Source:

    (1) Mano, M.M. Digital Design, 2nd Ed., Pearson Education, Asia Pte.

    Ltd., 2001.

  • 7/31/2019 001 Lab Manual

    64/115

    Digital Electronics

    Group Name: _________________

    Name: _________________________________

    A. Identify the ICs given to you:

    Ex. 343 Dual operational amplifier

    B. Draw the circuit diagram of the XOR gate you designed.

    C. Draw the truth table of the circuit and the schematic diagram.

  • 7/31/2019 001 Lab Manual

    65/115

    RC Filters

    Objective

    To introduce students to the different types of filters, specifically the RC filter

    circuit.

    RC Circuit

    A capacitor can store an electric charge while a resistor dissipates the flow of

    charges as heat. A fully charged capacitor, when connected across a resistive element, will

    lose its charge as current flows across the resistor. Connecting a voltage source across a

    series R-C circuit will cause a charging current to flow. This current changes with time as

    the voltages across the resistor and capacitor changes.

    By changing the source to a sine source, the frequency dependent voltage and

    current relationship in a capacitor can be exploited. The capacitor has a frequency-

    dependent resistance referred to as capacitive reactance. By combining resistors and

    capacitors in RC circuits, a frequency-dependent voltage divider circuit is realized. Thus

    is created a circuit in which the input and output relationships are frequency-dependent.

    These circuits form the basis of filters.

    Filters

    Fundamentally, all periodic fluctuations can be by a reduced to combination of sine

    waves of different frequencies. Electrical signals are no exception, and thus have their

    signature frequencies. In most cases, the frequency of the desired signal is known. Stray

    signals of different frequencies, or noise, interfere with the transmission of signals. Most of

  • 7/31/2019 001 Lab Manual

    66/115

    the time, these stray signals are unavoidably combined with the desired signal. However,

    there are ways to remove the noise from signal transmissions.

    Filters are used to weed out the unwanted signal frequencies. There are four basic

    types of filters. A low-pass filter only lets lower frequencies pass through. A high-pass

    filter lets higher frequencies pass through. A band-select filter only lets a certain range of

    frequencies to pass through. A band-reject filter lets all frequencies pass through except for

    a certain range of frequencies.

    In this lab, a simple RC filters characteristics are demonstrated.

    Exercise

    A. Construct the filter circuit shown below using CircuitMaker (Figure 1). The devices

    used are all under the .General Major Device Class:

    Signal Generator (.GeneralInstrumentsSignal Gen)

    Multimeter (.GeneralInstrumentsMultimeter)

    Note: Set to MeasureAC RMS

    Resistor (.GeneralResistorResistor)

    Capacitor (.GeneralCapacitorsCapacitor)

    Ground (.GeneralSourcesGround)

  • 7/31/2019 001 Lab Manual

    67/115

    AC V

    999.8mV

    AC V

    163.2mV

    C10.1uF

    1kHz

    V1-1.41/1.41V R1

    10k

    Figure 1. Filter circuit

    Double-click on the signal generator and set the Peak Amplitude to 1.414 V and the

    Frequency 1.000 kHz. Click the running man icon to run the analysis. When

    computation is finished the oscilloscope window appears. The cursor now becomes the

    oscilloscope probe. Shift-click to select the voltage input and voltage output nodes as

    indicated by the arrows on the following figure. If you do not press SHIFT while selecting,

    only the last selection will be plotted.

    Figure 2. Multimeter Device

    V out

    V in

  • 7/31/2019 001 Lab Manual

    68/115

    Figure 3. Oscilloscope window

    On the oscilloscope window, use the plot cursors to select specific points on the

    waves (Figure 3). The RMS amplitudes of the two test points are also given by the

    multimeters. Also, measure the phase shift between output and input. Adjust markers a

    and b (horizontally), and also c and d (vertically) to measure amplitudes and times,

    respectively. Write these data down.

    Click STOP to end simulation. Adjust the function generator frequency to 100 Hz.

    Again, turn the analysis on then measure the amplitudes and phase shifts of the two signals

    as before.

    Do the procedure for 10 Hz, 100 Hz, 160 Hz, 1kHz and 10 kHz frequencies. You

    can change the function generator frequency by double-clicking function generator and

    setting the variables as follows (Figure 4):

    Click and drag marker

    Marker measurements are displayed here

  • 7/31/2019 001 Lab Manual

    69/115

    Figure 4. Editing function generator variables.

    You must also setup analysis parameters as follows (Figure 5):

    Figure 5. Set-up analysis parameters.

    For Low frequency (100Hz and below), use the following set up (Figure 6):

  • 7/31/2019 001 Lab Manual

    70/115

    Figure 6. Low-frequency set-up

    The following settings might be better for f 1 KHz (Figure 7):

    Figure 7. Settings for frequency more than 1 kHz

    Bode Plot

    Edit the circuit to remove the multimeters. Select the voltage across the capacitor

    as a test point to display on the scope as shown below (Figure 8).

  • 7/31/2019 001 Lab Manual

    71/115

    C1

    0.1uF

    1kHz

    V1-1.41/1.41V R1

    10kV(3)

    Figure 8. Configuration for capacitor as test point.

    To set up and run an AC Analysis:

    1. Connect at least one Signal Generator to the circuit and enable it as an AC Analysis

    source. Do this by double-clicking the Signal Generator, clicking Wave, and setting up the

    AC Analysis Source options. Disable the other options (e.g. DC, Transient/Fourier,

    Multimeter)

    2. Choose Simulation > Analyses Setup > AC.

    3. Enter the AC Analysis settings (see the following figure), select the Enabled check box,

    and then choose OK.

    Sweep Option: What it Means

    Linear: Total number of Test Points in the sweep.

    Decade: Number of Test Points per decade in the sweep.

    Octave : Number of Test Points per octave in the sweep.

  • 7/31/2019 001 Lab Manual

    72/115

    Analysis setup:

    Figure 9. Analysis set-up.

    AC Analysis Setup:

    Figure 10. AC analysis set-up

    5. Run the simulation.

    Graph settings (click on the icon to edit graph settings). You should view:

    Magnitude (Linear Y Grid, Log X Grid and also Log X, Log Y)

    Phase in degrees (Linear Y Grid, Log X Grid)

  • 7/31/2019 001 Lab Manual

    73/115

    Figure 11. Graph settings.

    Note how the AC Analysis rapidly confirms the step-by-step determinations that you did

    earlier.

    B. Swap the positions of the resistor and capacitor. Again, get the amplitudes and

    phase shifts of the signals at 10 Hz, 100 Hz, 160 Hz, 1kHz and 10 kHz. Also obtain the

    Bode plot as above.

    Source:

    (1) Boylestad, R.L.; Nashelsky, L. Electronic Devices and Circuit Theory, 8th Ed.,

    Prentice Hall, 2002.

  • 7/31/2019 001 Lab Manual

    74/115

    RC Filters

    Group Name: _________________

    Name: ______________________________

    A.

    Frequency Vin Vout Vout / Vin Phase shift

    10 Hz

    100 Hz

    160 Hz

    1 kHz

    10 kHz

    1. Using the data above, plot the frequency response in the graphs provided.

    2. What type of filter is this? ____________________

    3. In the Bode plot window, use the markers to find the frequency where Vout = 0.707

    Vin. Frequency = _______Hz. Compare this with fc =1/(2RC).

    4. In the Bode plot of phase versus frequency, what is the phase shift at this frequency?

    Phase shift = ______________ degrees (indicate sign)*.

    5. Encircle your answer: In this circuit, Vout lags/leads Vin .

    B. (after swapping R and C)

  • 7/31/2019 001 Lab Manual

    75/115

    Frequency Vin Vout Vout / Vin Phase shift

    10 Hz

    100 Hz

    160 Hz

    1 kHz

    10 kHz

    6. Using the data above, plot the frequency response in the graphs provided.

    7. What type of filter is this? ____________________

    8. In the Bode plot window, use the markers to find the frequency where Vout = 0.707

    Vin. Frequency = _______Hz. Compare this with fc =1/(2RC).

    9. In the Bode plot of phase versus frequency, what is the phase shift at this frequency?

    Phase shift = ______________ degrees (indicate sign)*.

    10. Encircle your answer: In this circuit, Vout lags/leads Vin .

    *Compute phase shift as follows: (degrees) = t * f / 360

    Where:

    t = time delay between input and output waveform in seconds

    f = frequency in Hz

    A. Graphs of frequency response:

  • 7/31/2019 001 Lab Manual

    76/115

    B. Graphs of frequency response:

    Frequency response of RC filter: Magnitude

    Type: _____ - pass

    00.10.20.30.40.50.60.70.80.9

    1

    10 100 1000 10000

    Frequency (Hz)

    Magnitude(Vout/

    Frequency response of RC filter: Phase

    Type: _____ - pass

    -90

    -45

    0

    45

    90

    10 100 1000 10000

    Frequency (Hz)

    Phase

    (degre

  • 7/31/2019 001 Lab Manual

    77/115

    B. Graphs of frequency response.

    Frequency response of RC filter: Magnitude

    Type: _____ - pass

    0

    0.10.20.30.40.50.60.70.80.9

    1

    10 100 1000 10000

    Frequency (Hz)

    Magnitude(Vout/

    Frequency response of RC filter: Phase

    Type: _____ - pass

    -90

    -45

    0

    45

    90

    10 100 1000 10000

    Frequency (Hz)

    Phase

    (degre

  • 7/31/2019 001 Lab Manual

    78/115

    Microcontroller I: ADC

    Objectives

    (1) To introduce students to data acquisition using a microcontroller.

    (2) To familiarize students on microcontroller peripherals, particularly the analog-to-

    digital converter (ADC).

    The Zilog Encore!TM Miniboard

    Encore PLCC Mini Board (Figure 1) is a module that utilizes the on-chip

    peripherals of the Z8F6401 Flash Microcontroller, like the eight-channel Analog-to-Digital

    Converter (ADC) and the Universal Asynchronous Receiver/Transmitter. The board has a

    64-K flash memory and is powered using a 9VDC adapter. This module uses pin headers to

    access the input/output pins of Z8F6401.

    Figure 1. PLCC Miniboard

  • 7/31/2019 001 Lab Manual

    79/115

    The ZDS II Encore Software

    The Zilog Development Studio II has an integrated development environment and

    has a built-in C compiler, assembler, linker and project manager. A debugger allows

    single-stepping, viewing of variables, register files, code/data memory, ports and timers.

    The ZDS II connects to the microcontroller (uC) via serial port communications. When

    programming in the ZDS II environment, the user should know these ZDS II basics:

    A. Creating a New Project

    To start a new project (Figure 2) in ZDS II environment, click File and choose,

    New Project.

    Figure 2. New Project Window

    Select target, CPU and Project Type as shown above. After that, select the location

    for the new folder and write the folder name for the new project. Finally, type the filename

    for the new project (Figure 3).

  • 7/31/2019 001 Lab Manual

    80/115

    Figure 3. New folder for new project

    In the New Project window, click continue and wait for the Configure New

    Project window to appear (Figure 4). Make sure that C Runtime Library and Floating

    Point library are selected. After that, select startup module, dynamic frames and large

    memory model.

    Figure 4. Configure New Project Dialog Box

    Click next, then review target memory configuration. Make sure that the settings are the

    same as that shown in Figure 5, then click Finish.

  • 7/31/2019 001 Lab Manual

    81/115

    Figure 5. Configuring New Project

    To check target system settings, click on Project then Settings and select the

    Debugger tab (Figure 6). Make sure that the Z8 Encore! OCD Driver is selected. Else,

    click on Configure Driver and change to the appropriate setting. Click on the C tab

    and make sure the appropriate settings are made in the General category, particularly

    disable optimizations. (Figure 7)

    Figure 6. Debugger Tab in Project Setting Dialog Box.

  • 7/31/2019 001 Lab Manual

    82/115

    Figure 7. C Tab in Project Setting Dialog Box.

    In the Preprocessor category, add __Z8F640 in the preprocessor definitions (Figure 8).

    Figure 8. Preprocessor Definitions.

    B. Creating a New Source Code File

    To create a source code file, click File then select New File (Figure 9). After

    coding in C, click File then select Save As and write the filename with a .c

    extension. Make sure that the file is saved in the folder for the project. To create source

    code file, choose Project Files then right click. Select Add Files to Project. Choose

    the .c file of choice (Figure 10).

  • 7/31/2019 001 Lab Manual

    83/115

    Figure 9. New Source Code File

    Figure 10. Add Files to Project

    Figure 11 shows some of the shortcuts worth mentioning. Compile means

    converting source code into op-codes / object code / machine code. Link, on the other hand

    pertains to combining all these object codes. Build is tantamount to compiling followed by

    linking. Syntax errors appear in the output window (Figure 12). Double-clicking on an

    error message takes the programmer to the offending line.

  • 7/31/2019 001 Lab Manual

    84/115

    Figure 11. Shortcut Icons

    Figure 12. Output Window

    Exercise

    In this exercise, you will input varying voltage into one of the analog inputs of the

    Miniboard and obtain the digital output using Hyperterminal serial communications

    program. This output is compared to the voltage input measured by a multimeter.

    In interfacing the Encore PLCC Mini Board to a PC, RS-232 or serial

    communication is used. A program (adc.c) written in C can be downloaded into the 64-K

    flash memory via a serial cable from COM 1 (9-pin) to Debugger UART. To output data

    generated by the Z8F6401, it is necessary to connect the Console UART to COM 2 (9 or

    25-pin). In case COM 2 is 25-pin, a 9-to-25 serial cable should be employed.

    IMPORTANT NOTE: Ask the instructor to interface the Miniboard to the PC

    and to provide the text file of adc.c. Copy-paste this code to the New Source Code File

    window.

  • 7/31/2019 001 Lab Manual

    85/115

  • 7/31/2019 001 Lab Manual

    86/115

    Sources:

    (1) De Vera, I.M.S. Laboratory Data Acquisition System Based on the Z8 Encore!TM

    Microcontroller. 2006.

    (2) De Vera, I.M.S.; Chainani, E.T. Low Cost Laboratory Data Acquisition System

    Based on the Z8 Encore!TM Microcontroller for pH Measurement. Kimika, 22, 2, 97-

    83, 2006.

    (3) Sison, L.G.; Burgos, O.T. Microcontroller for Data Acquisition and Motor

    Control. 2005.

    Microcontroller I: ADC

    Group Name: _________________

  • 7/31/2019 001 Lab Manual

    87/115

    Name: _________________________________

    A. Draw your potentiometer-potential divider circuit design here.

    B. Comparison of Analog input and ADC output

    Nominal Analog

    Input (V)

    Actual Analog Input

    (V)

    ADC Output from

    Hyperterminal (V)

    % Difference

    0.025

    0.050

    0.075

    0.100

    0.200

    0.300

    0.400

    0.5001.00

    1.25

    1.50

    1.75

    2.00

    2.25

    2.50

    2.75

    3.00

    1. How is analog-to-digital conversion performed? Focus your research on the

    algorithm used by sigma-delta ADCs (the ADC used by the Z8F6401

    microcontroller).

  • 7/31/2019 001 Lab Manual

    88/115

    2. Plot decimal equivalent of the ADC output vs. voltage input for two voltage ranges:

    0.025 to 0.500-V and 1.00 to 3.00-V. Take note of the linearity coefficient and the

    slope of the plots (submit worksheet and graph separately). What can you say

    about the sensitivity of the ADC as the analog input increment becomes smaller?

    Comment on the accuracy of ADC conversion as the input approaches zero (i.e.

    100 mV down to 25 mV).

    3. Determine the step-size of the ADC (voltage change needed for ADC value to

    change by one unit).

  • 7/31/2019 001 Lab Manual

    89/115

    Microcontroller II: Sensor

    Objective

    To create a Z8 Encore!TM based pH measurement system using a glass electrode.

    pH Measurements using a Glass Electrode

    The glass electrode is undisputedly the most important indicator electrode for

    hydrogen ion. It is convenient to use and subject to few of the interferences that affect

    other pH-sensing electrodes. One of the most important developments in chemical

    instrumentation over the past three decades has been the advent of compact, inexpensive,

    versatile integrated-circuit amplifiers (op-amps). These devices allow us to make potential

    measurements on high-resistance cells, such as those that contain a glass electrode, without

    drawing appreciable current. Even a small current (10-7 to 10-10 A) in a glass electrode

    produces a large error in the measured voltage due to loading and electrode polarization.

    Framework

    This experiment can be more understood by looking at the block diagram in Figure

    1.

    Host PC or

    PDAZ8F6401 uC

    ADC

  • 7/31/2019 001 Lab Manual

    90/115

  • 7/31/2019 001 Lab Manual

    91/115

    Design an amplifier circuit using op-amp A in LF353N (see Figure 2, Expt. 6),

    which can amplify the incoming analog signal from the glass electrode by a factor of 8.3.

    Put a 0.1 uF non-polarized capacitor between the output and the inverting input of the

    amplifier.

    Using a BNC connector, connect the glass electrode to the non-inverting input of

    this op-amp. Make the necessary tests if the amplifier circuit is working.

    A.3 Level Shifter

    Figure 2 shows the level shifter circuit. Implement this circuit on your bread board.

    If one measures the amplified voltage (output of A.2), negative values above pH 7

    will be obtained. This signal is not fit as an ADC input. (Why?). Thus, the amplified

    analog signal needs to be level-shifted to positive voltage values. A voltage-follower is

    implemented via op-amp B in LF353N. Consequently, Vshift is equal to VCC. An external

    voltage reference set to 3.3 V (designated as VCC in Fig. 2 , see also Fig. 1, Expt. 9) is

    employed. Note of the label amplifier output in figure 2. This is where you connect the

    amplifier output. VDD in the same figure is pin 21 of the Miniboard.

    Inspect Figure 2 thoroughly. Justify that the signal is indeed level-shifted to

    positive values and that the following equation can be derived from your amplifier circuit

    design and the level shifter:

    2

    ]30.3)27.8*[( +=

    VinVout Equation 1

  • 7/31/2019 001 Lab Manual

    92/115

    Moreover, test your circuit if the output abides Equation 1. The level-shifted signal (Vout)

    will now serve as the input to ANA0 of the ADC.

    Figure 2. Level Shifter

    B. Interfacing the Miniboard and Loading the software

    As before, ask the instructor to interface the PLCC miniboard to the PC. Open the

    file pHmeter.c using ZDS II (refer to Experiment 9 for procedures). Click the following

    icons in succession: CompileBuildConnect to TargetDownloadGo. Make sure

    that Hyperterminal is on-line.

    C. Making pH measurements

    Vcc (3.30 V)

    Vout

    Vshift

    VDD

  • 7/31/2019 001 Lab Manual

    93/115

    The groups will share the standard buffer solutions for the calibration phase. Each

    group will receive three unknowns. Your task is to get the pH of the unknown solutions

    using your groups pH meter and compare this to the pH measurement obtained by using

    a commercial pH meter (i.e. Sartorius).

    Sources:

    (1) De Vera, I.M.S. Laboratory Data Acquisition System Based on the Z8 Encore!

    TM Microcontroller. 2006.

    (2) De Vera, I.M.S.; Chainani, E.T. Low Cost Laboratory Data Acquisition System

    Based on the Z8 Encore!TM Microcontroller for pH Measurement. Kimika, 22, 2,

    97-83, 2006.

    (3) Sison, L.G.; Burgos, O.T. Microcontroller for Data Acquisition and Motor

    Control. 2005.

  • 7/31/2019 001 Lab Manual

    94/115

    Microcontroller II: Sensor

    Group Name: _________________

    Name: _________________________________

    Calibration Phase

    pH Standard Buffer Decimal Value of ADC

    Output

    Voltage Equivalent

    4.00

    7.00

    10.00

    pH Measurements

    Unknown pH Miniboard pH Sartorius % difference

    1

    2

    3

    1. Draw your amplifier circuit design here.

    2. (a) The 0.1 uF capacitor in the amplifier circuit acts as what type of filter?

    Calculate the cut-off frequency.

  • 7/31/2019 001 Lab Manual

    95/115

    (b) The 10 uF capacitor parallel to the output of the level shifter is similar to the

    filter in (a). Calculate its cut-off frequency.

    3. Prove Equation 1.

    4. Plot the pH calibration curve (decimal equivalent of ADC output vs. voltage in V)

    in Excel or simply determine the linearity coefficient using your calculator.

    Which is better, a three-point or a two-point calibration? Why?

  • 7/31/2019 001 Lab Manual

    96/115

    5. Account for the difference between the pH measurements made using the

    microcontroller-based pH meter and the commercial pH meter (Sartorius).

    Evaluate the accuracy and precision of measurements using the microcontroller-

    based pH meter.

    6. What are the factors that may lead to errors in pH measurements?

    Appendix A: Soldering

  • 7/31/2019 001 Lab Manual

    97/115

    Soldering is accomplished by quickly heating the metal parts to be joined, and then

    applying aflux and asolder to the mating surfaces. The finished solder joint metallurgically

    bonds the parts forming an excellent electrical connection between wires and a strong

    mechanical joint between the metal parts. Heat is supplied with a soldering iron or other

    means. The flux is a chemical cleaner which prepares the hot surfaces for the molten

    solder. The solder is a low melting point alloy of non-ferrous metals.

    Soldering gun or iron

    A soldering iron is an electric hand tool that joins two pieces of metals by fusing

    their surfaces together using a metal alloy known as solder. Usually, for electronics, the

    solder used is an alloy composed primarily of lead. A soldering iron will

    melt the lead by applying constant heat to it. This melted lead, once it dries,

    joins the two metal surfaces together.

    A soldering gun operates with the same principle as a soldering iron,

    but pressing its trigger can increase its heat.

    Be careful in using a soldering tool, since it operates at high temperatures. Do not

    play around with it. Also, do not inhale the smoke coming from soldering action, as it

    contains irritants to mucous membranes.

    Soldering lead

  • 7/31/2019 001 Lab Manual

    98/115

    Solder is a metal or metallic alloy used, when melted, to join

    metallic surfaces together. The most common alloy is some

    combination of tin and lead. Certain tin-lead alloys have a lower

    melting point than the parent metals by themselves. The most common alloys used for

    electronics work are 60/40 and 63/37. The chart below shows the differences in melting

    points of some common solder alloys.

    Tin/Lead Melting Point

    40/60 460 degrees F (230 degrees C)

    50/50 418 degrees F (214 degrees C)60/40 374 degrees F (190 degrees C)

    63/37 364 degrees F (183 degrees C)

    95/5 434 degrees F (224 degrees C)

    The eutecticum is the point where the melting point and solid point is the same and the

    melting point is lower then the melting point of the individual metals used in the alloy. The

    eutectic point in tin/lead alloy is 61.9% tin and 38.1% lead (if metals are 100% pure).

    60/40 solder is commercially available and is recommended for solder work.

    With non-eutectic alloys a paste-phase develops in the zone between the liquid and solid

    line. In theory this could result in soldering failures if the solder joint in this paste-phase

    undergoes mechanical stress or gets serious vibration. Small tolerances from the eutectic

    point have little influence in the soldering process because of fast cooling.

  • 7/31/2019 001 Lab Manual

    99/115

    Most soldering jobs can be done with flux-cored solder (solder wire with the

    flux in the center) when the surfaces to be joined are already clean or can be

    cleaned of rust, dirt and grease. Flux can also be applied by other means (it is

    also sold separately in tin cans). Flux only cleans oxides off the surfaces to be soldered. It

    does not remove dirt, soot, oils, silicone, etc.

    Base Material

    The base material in a solder connection consists of the component lead and the plated

    circuit traces on the printed circuit board. The mass, composition, and cleanliness of the

    base material all determine the ability of the solder to flow and adhere properly (wet) and

    provide a reliable connection.

    If the base material has surface contamination, this action prevents the solder from wetting

    along the surface of the lead or board material. A surface finish usually protects component

    leads. The surface finishes can vary from plated tin to a solder - dipped coating. Plating

    does not provide the same protection that solder-coating does because of the porosity of the

    plated finish, thus the component wire may develop oxides.

  • 7/31/2019 001 Lab Manual

    100/115

    The Correct Way to SolderSome Reasons for Unwettability

    1. The component lead has developed an oxide. Normally this can be removed by the

    flux, but a thick layer of oxidation requires removal by sandpaper or other

    mechanical means.

    2. The selected temperature is too high. The tin coating is burnt off rapidly and

    oxidation occurs.

    3. Oxidation may occur because of wrong or imperfect cleaning of the tip: when other

    material is used for tip cleaning instead of the original damp Weller sponge. A

    damp cellulose sponge is recommended; other sponges, rags or cloth will melt or

    burn.

    4. Use of impure solder or solder with flux interruptions in the flux core.

    5. Insufficient tinning when working with high temperatures over 665 degrees F (350

    degrees C) and after work interruptions of more than one hour.

    6. A "dry" tip, i.e. the tip is allowed to sit without a thin coating of solder oxidation

    occurs rapidly.

    7. Use of fluxes that are highly corrosive and cause rapid oxidation of the tip (e.g.

    water soluble flux).

    8. Use of mild flux that does not remove normal oxides off the tip (e.g. no-clean flux).

  • 7/31/2019 001 Lab Manual

    101/115

    The Soldering Iron Tip

    The soldering iron tip transfers thermal energy from the heater to the solder

    connection. In most soldering iron tips, the base metal is copper or some copper alloy

    because of its excellent thermal conductivity. A tip's conductivity determines how fast

    thermal energy can be sent from the heater to the connection.

    Both geometric shape and size (mass) of the soldering iron tip affect the tip's

    performance. The tip's characteristics and the heating capability of the heater determines

    the efficiency of the soldering system. The length and size of the tip determines heat flow

    capability while the actual shape establishes how well heat is transferred from the tip to the

    connection.

    There are various plating processes used in making soldering iron tips. These

    plating operations increase the life of the tip. The figure below illustrates the two types of

    plating techniques used for soldering iron tips. One technique uses a nickel plate over the

  • 7/31/2019 001 Lab Manual

    102/115

    copper. Then, an iron electroplate goes over the nickel. The iron and the nickel create a

    barrier between the copper base material and tin used in the solder alloy. The barrier

    material prevents the copper and tin from mixing together. Nickel-chrome plating on the

    rear of the tip prevents solder from adhering to the back portion of the tip (which could

    cause difficulty in tip removal) and provides a controlled wetted area on the iron tip.

    Another plating technique is similar but omits the nickel electroless plating, leaving the

    iron to act as the barrier metal.

    How to Care For Your Tip

    Because of the electro-plating Weller tips should never be filed or ground. Weller

    offers a large range of tips and there should be no need for individual shaping by the

    operator.

    Although Weller tips have a standard pre-tinning (solder coating) and are ready for

    use, it is recommended that you pre-tin the tip with fresh solder when heating it up the first

    time. Any oxide covering will then disappear. Tip life is prolonged when mildly activated

    rosin fluxes are selected rather than water soluble or no-clean chemistries.

    When soldering with temperatures over 665 degrees F (350 degrees C) and after

    long work pauses (more than 1 hour) the tip should be cleaned and tinned often, otherwise

    the solder on the tip could oxidize causing unwettability of the tip. To clean the tip use the

    original synthetic wet sponges from Weller (no rags or cloths).

    When doing rework, special care should be taken for good pre-tinning. Usually

    there are only small amounts of solder used and the tip has to be cleaned often. The tin

  • 7/31/2019 001 Lab Manual

    103/115

    coating on the tip could disappear rapidly and the tip may become unwettable. To avoid

    this the tip should be re-tinned frequently.

    Additional Tip and Tiplet Care Techniques

    Listed below are suggestions and preventative maintenance techniques to extend life and

    wettability of tips and desoldering tiplets.

    1. Keep working surfaces tinned, wipe only before using, and return immediately.

    Care should be taken when using small diameter solder to assure that there is

    enough tin coverage on the tip working surface.

    2. If using highly activated rosin fluxes or acid type fluxes, tip life will be reduced.

    Using iron plated tips will increase service life.

    3. If tips become unwettable, alternate applying flux and wiping to clean the surface.

    Smaller diameter solders may not contain enough flux to adequately clean the tips.

    In this case, larger diameter solder or liquid fluxes may be needed for cleaning.

    Periodically remove the tip from your tool and clean with a suitable cleaner for the

    flux being used. The frequency of cleaning will depend on the frequency and type

    of usage.

    4. Filing tips will remove the protective plating and reduce tip life. If heavy cleaning

    is required, use a Polishing Bar available from your distributor.

    5. Do not remove excess solder from a heated tip before turning off the iron. The

    excess solder will prevent oxidation of the wettable surface when the tip is

    reheated.

  • 7/31/2019 001 Lab Manual

    104/115

  • 7/31/2019 001 Lab Manual

    105/115

    temperature when the most commonly used solders have a melting point under 400 degrees

    F. Using a higher temperature stores heat in the tip, which speeds up the melting process.

    The operator can then complete the solder connection without applying too much pressure

    on the joint. This practice also allows a proper formation of an intermetallic layer of the

    parts and solder. This is critical for reliable electrical and mechanical solder joints.

    The Operator's Effect on the Process

    The operator has a definite effect on the manual soldering process. The operator

    controls the factors during soldering that determine how much of the soldering iron's heat

    finally goes to the connection.

    Besides the soldering iron configuration and the shape of the iron's tip, the operator

    also affects the flow of heat from the tip to the connection. The operator can vary the iron's

    position and the time on the connection, and pressure of the tool against the pad and lead of

    the connection.

    When the tip of the iron contacts the solder connection, the tip temperature

    decreases as thermal energy transfers from the tip to the connection. The ability of the

    soldering iron to maintain a consistent soldering temperature from connection to

    connection depends on the iron's overall ability to transfer heat as well as the operator's

    ability to repeat proper technique.

    The Reliable Solder Connection

  • 7/31/2019 001 Lab Manual

    106/115

    Two connection elements must properly function for a solder joint to be reliable.

    The solder within the connection must mechanically bond the component to the PCB. The

    connection must also provide electrical continuity between the device and board. The

    proper intermetallic layer assures both.

    Mechanical

    In surface mount and nonclinched through-hole technology, the solder provides the

    mechanical strength within the connection. Important factors for mechanical strength

    include the wetting action of the solder with the component and board materials, physical

    shape and composition of the connection, and the materials' temperature within the

    connection during the process. The connection temperature should not be too high, causing

    embrittlement, or too low, resulting in poor wetting action.

    Electrical

    If a solder connection is mechanically intact, it is considered to be electrically

    continuous. Electrical continuity is easily measured and quantified.

    Testing Reliability

    Two easily measured indicators in the soldering process that can determine the

    reliability of the solder connection are the soldering iron's tip temperature and the solder's

    wetting characteristics. The tip's temperature during the soldering process is an indicator of

  • 7/31/2019 001 Lab Manual

    107/115

    the amount of heat being transferred from the tip to the connection. The optimum rate of

    heat transfer occurs if the soldering iron tip temperature remains constant during the

    soldering process.

    Another indicator for determining reliability is the solder's wetting action with the

    lead and board materials. As operators transfer heat to the connection, this wetting

    characteristic can be seen visually. If the molten solder quickly wicks up the sides of the

    component on contact, the wetting characteristic is considered good. If the operator sees

    the solder is flowing or spreading quickly through or along the surface of the printed circuit

    assembly, the wetting is also characterized as good.

    Right Amount of Solder

    a) Minimum amount of solder

    b) Optimal

    c) Excessive solder

    Solderability

  • 7/31/2019 001 Lab Manual

    108/115

    a) Bad solderability of terminal wire

    b) Bad soldering of PCB

    c) Bad soldering of terminal wire and PCB

    Key Points to Remember

    1. Always keep the tip coated with a thin layer of solder.

    2. Use fluxes that are as mild as possible but still provide a strong solder joint.

    3. Keep temperature as low as possible while maintaining enough temperature to

    quickly solder a joint (2 to 3 seconds maximum for electronic soldering).

    4. Match the tips