OP AMP Application Part 1 (Electronics 2) — Transcript
Full transcript
- 0:00hi hello um this video is
- 0:03um about op amp or operational
- 0:05amplifiers
- 0:07practical applications okay so to start
- 0:10with
- 0:11um we have here the negative uh sorry
- 0:14the inverting amplifier or what we call
- 0:16the negative scaler
- 0:17okay so um inverting amplifier so your
- 0:21operational amplifier can work as an
- 0:23inverting amplifier or a negative scaler
- 0:26so this is a closed loop gain of an in
- 0:30of the inverting amplifier depends on
- 0:32the ratio
- 0:33of the two external resistors which are
- 0:36your
- 0:36r1 and your rf okay and it is
- 0:39independent of the amplifier parameters
- 0:42okay so that means um uh it doesn't
- 0:44matter if your amplifier or your op amp
- 0:47is 741 or other type of op amps okay
- 0:50but when we connect it in an inverting
- 0:53amplifier mode
- 0:54so the gain will only be determined by
- 0:57your r1 and your
- 0:59rf okay so it means it scales the input
- 1:03or it multiplies an input so it's like a
- 1:06multiplier okay so it scales the input
- 1:09it multiplies the input by a minus
- 1:12constant factor
- 1:14of k okay so this is our
- 1:18um this is our representation for an
- 1:21inverting amplifier so this is your
- 1:22feedback resistance and this is your r1
- 1:25or the internal resistance so for
- 1:27inverting amplifier our input
- 1:30is being placed or being um uh
- 1:34being applied at the inverting terminal
- 1:36so for
- 1:37741 our inverting terminal is your pin
- 1:40number
- 1:41two okay so your non-inverting input
- 1:44is grounded so our formula
- 1:48for the voltage gain is uh the output
- 1:50voltage divided by your
- 1:52input voltage
- 1:55okay so um that is equivalent to
- 1:59negative rf all over one so from our
- 2:01previous video we have already derived
- 2:04why it became um negative rf all over r1
- 2:08so your rf all over r1 can be um
- 2:12represented by a constant okay so let us
- 2:15let us call that k
- 2:16so that means your input voltage can be
- 2:20multiplied
- 2:21k times okay so k times but we have a
- 2:24negative sign here
- 2:26showing that there is a 180 degrees out
- 2:29of phase
- 2:30between your input and your output
- 2:32signals
- 2:33okay so uh
- 2:37another application for our operational
- 2:40amplifier
- 2:41is as a non-inverting amplifier or what
- 2:44we call the positive scalar
- 2:46okay so this is used when there is a
- 2:49need for an output
- 2:50which is equal to the input multiplied
- 2:53by a positive
- 2:54constant okay so positive scalar circuit
- 2:58which uses negative feedback but
- 3:01provides an
- 3:01output equals the input multiplied by
- 3:04opacity of
- 3:05constant so there is uh no 180 degrees
- 3:09phase reversal or your output is in
- 3:11phase
- 3:12with your input okay so this is our
- 3:14representation for a non-inverting
- 3:16amplifier
- 3:17so we apply your input voltage as at the
- 3:21non-inverting terminal so if we are
- 3:23using the 741 operational amplifier
- 3:26this is your pin number three okay so
- 3:29this is
- 3:29still your feedback resistance which is
- 3:32your rf and this
- 3:33is still your r1 however our
- 3:37inverting terminal here is
- 3:40grounded okay so our voltage gain
- 3:43still equal to v output divided by v
- 3:47input and our um value for our
- 3:51gain is equal to r1 plus rf divided by
- 3:55r1 or we can simplify that as
- 3:57one plus rf all over r1
- 4:00so this is our gain for a non-inverting
- 4:03amplifier okay now um we have this
- 4:07cast that when your input is placed at
- 4:10the
- 4:10at the non-inverting terminal okay
- 4:14so our inverting terminal
- 4:19uh if our input is placed at our
- 4:21inverting terminal our non-inverting
- 4:23terminal has no resistance or it is
- 4:26simply grounded
- 4:27or if our input was placed in the
- 4:30non-inverting terminal
- 4:31the the input resist the input voltage
- 4:34is directly
- 4:35coupled to your operational amplifier
- 4:38however in practice we have this what we
- 4:41call bias compensating resistance so if
- 4:44you can still remember
- 4:45from our previous um video okay so there
- 4:49are such things
- 4:50as uh our input uh bias currents
- 4:54and our input offset currents that are
- 4:56already within your
- 4:58integrated uh within your operational
- 5:01amplifier
- 5:01so what does that mean so it means that
- 5:04um even though we do not have
- 5:05any input yet we can already read
- 5:08something at the output
- 5:10okay so there is already an output
- 5:12voltage even though we don't have any
- 5:13input signal
- 5:14and we don't like that okay so um
- 5:18but we cannot totally remove those
- 5:20because those are already
- 5:22inside okay or within your operational
- 5:25amplifier
- 5:26so what do we with what can we do is by
- 5:29applying a potentiometer okay so that is
- 5:32our nulling resistance
- 5:34and another thing is by applying what we
- 5:37call the bias compensating
- 5:40resistance okay or our rc
- 5:43okay so our rc represents
- 5:46all or a portion of the resource
- 5:48resistance
- 5:49so the exact value of rc is not critical
- 5:52because we do not usually make use of
- 5:54your rc in computing for your gain
- 5:57okay and the closest standard value is
- 6:00usually sufficient
- 6:02okay so for example this is now our
- 6:05inverting um
- 6:06amplifier circuit previously this is
- 6:09just grounded
- 6:10but in uh in actual okay in practical
- 6:13applications
- 6:14we place here an rc so what is the value
- 6:17of our rc in our design
- 6:19so your gain will still be um will still
- 6:22be dictated by the value of the rf and
- 6:25our
- 6:25r1 here but your rc here is just the
- 6:28parallel combination of your rf and your
- 6:32rl so in case there is no exact standard
- 6:35value
- 6:37for this parallel combination so it is
- 6:39okay we just have to choose the closest
- 6:42standard value okay so this is now the
- 6:45new
- 6:45um representation or the new schematic
- 6:48diagram for our
- 6:50non-inverting amplifier so um previously
- 6:54we don't have any resistor here it's
- 6:56just directly
- 6:57the input is just directly connected to
- 6:59the non-inverting terminal of your op
- 7:02amp but uh in practical use we place a
- 7:05biasing compensating resistance
- 7:07and that is still equivalent to the um
- 7:11parallel combination of your rf and your
- 7:14ri
- 7:14okay so we have here some design
- 7:18considerations okay
- 7:20so a summary of some of the major dis
- 7:22considerations of the simplified
- 7:25design approach to operational amplifier
- 7:28small signal amplifier circuits
- 7:30are as follows so number one be sure
- 7:33that the dynamic
- 7:34range of the op amp based on power
- 7:37supply levels with some back off
- 7:39will be sufficient for the desired
- 7:42output signal
- 7:43so that this uh if you can still
- 7:45remember for a 741
- 7:48you can um you can make use of
- 7:51a power supply having a value of
- 7:54positive or negative 12 volts so since
- 7:57your operational amplifier
- 7:59is dual um dual supply so you have a
- 8:02positive and a negative voltage
- 8:04so it can be positive 12 okay plus or
- 8:07minus 12 it can be plus or minus 9 volts
- 8:10it can be plus or minus 15 plus or minus
- 8:1318 okay so in your design you should be
- 8:17um you should be aware okay
- 8:20on the actual power supply level so for
- 8:23example
- 8:23you are you need in your design to have
- 8:26an output equivalent to
- 8:2812 volts okay so if
- 8:31your output must be equivalent to 12
- 8:34volts
- 8:34you will not be using any value which is
- 8:37lower than 12 volts or even
- 8:39exact 12 volts why because uh
- 8:42we we discussed um on our previous uh
- 8:46video that there are some back off
- 8:50okay for that specific voltage so if we
- 8:53have a
- 8:54for example 12 maybe we can
- 8:57have a maximum of output of just 10
- 9:00volts okay so if you will be needing 12
- 9:02volts
- 9:03it will not be sufficient so if we will
- 9:05be needing an output which is equal to
- 9:0712 volts
- 9:08better we make use of a supply which is
- 9:11equivalent to plus or minus 15 or plus
- 9:14or minus
- 9:1418 and so on okay so your design must be
- 9:18practical so your design must be um
- 9:23what you call this you have to use um
- 9:27the proper supply power supply levels in
- 9:30your desired
- 9:31output signal okay so whenever number
- 9:34two whenever possible choose resistance
- 9:36values in the range of
- 9:38one kilo ohms to 100 kilo ohms
- 9:41okay so our our
- 9:46ideal value from our previous video
- 9:50was 10 kilo ohms okay so
- 9:53except avoid resistances that load the
- 9:57output in the lower portion of the range
- 9:59that means values of 10 kilo ohm
- 10:03and greater are most widely used for
- 10:05many applications because if we make use
- 10:07of a lower value
- 10:09um our
- 10:12back off in our power supply will also
- 10:17become lower
- 10:18okay so if if our 15 volts for example
- 10:22uh will give us an output of positive
- 10:25plus or minus uh 13 volts um if we make
- 10:29use of our resistance which is lower
- 10:31than kilo ohms
- 10:32we might get a lower supply valve
- 10:35voltage okay
- 10:36so number three you have to limit the
- 10:38magnitudes
- 10:39of closed loop gain to values much
- 10:42smaller than the available open loop
- 10:44gain so that's the main purpose of our
- 10:46feedback resistance
- 10:48okay so that is the the reason why we
- 10:51place a
- 10:52feedback resistance so that we can lower
- 10:55down
- 10:56our open loop gain which is equivalent
- 10:59to 100
- 11:00000 for an operational amplifier so
- 11:03typically closed loop gain magnitudes
- 11:06are kept under 100
- 11:08okay and finally we have to check the
- 11:11maximum output current levels under
- 11:13worst case condition
- 11:15okay so each operational amplifier has
- 11:18its maximum um
- 11:21output current so four seven four one so
- 11:24it is 25 milli amperes so
- 11:27we might uh we might um
- 11:31over uh we have we might uh use
- 11:34okay a maximum current greater than
- 11:38its uh level its maximum level
- 11:42okay which can um destroy or ruin your
- 11:46operational amplifiers okay so for the
- 11:49resistor values
- 11:50um this are the most widely used so
- 11:54this are you you must at least be
- 11:56familiar
- 11:57with this values okay so this is the
- 11:59most widely used resistors okay so
- 12:02they are low powered actual lead carbon
- 12:05composition and film resistors with
- 12:07tolerance of 5
- 12:09and ten percent okay all the values
- 12:12listed are available
- 12:13in five percent tolerance but only the
- 12:15bold face values are available in
- 12:1810 tolerances okay so if you can still
- 12:22remember your
- 12:23um resistor color coding okay so what do
- 12:26we mean by this so when we say
- 12:2810 so this is available in one kilo ohm
- 12:3210 kilo ohms 100 kilo ohms okay so 10k
- 12:36um one mega okay so those are in those
- 12:39following range so you have
- 12:401.5 k okay so you have
- 12:44um 15k okay so 150 kilo ohms like that
- 12:50okay so
- 12:52for other applications practical
- 12:55applications such as instrumentations
- 12:57okay we're in
- 12:58we are very particular with our design
- 13:01and we do not want any variations or
- 13:05high variations in our design we also
- 13:08have
- 13:08resistor values in one percent
- 13:11tolerances okay so
- 13:13if we're going to make use of this
- 13:14resistor values so they have a tolerance
- 13:17of one percent only so therefore
- 13:19you have of uh the the possibility of
- 13:23getting an accurate circuit is higher
- 13:27because your tolerance is very very
- 13:29small okay so usually these are being
- 13:31used for instrumentation
- 13:33purposes so the design problem actually
- 13:37design problems are not very very
- 13:39difficult because
- 13:40when you say inverting amplifier you
- 13:42have already the design for an
- 13:44inverting amplifier you know already
- 13:47what does an inverting amplifier looks
- 13:49like
- 13:49okay so when we say design actually
- 13:53you're just um placing your value
- 13:57of rf and r1 in such a way that you are
- 14:01um
- 14:02you are asked for
- 14:05okay so what what must be the value of
- 14:08rf and r1 that is being required in the
- 14:12design okay
- 14:13so we have here an example using a five
- 14:17percent
- 14:18resistance values okay design and
- 14:20inverting so vcvs is a voltage
- 14:23controlled voltage
- 14:24source um amplifier okay
- 14:27to provide a voltage gain of negative 10
- 14:30so we want a voltage gain of negative 10
- 14:33and what are some other considerations
- 14:36so it says here that the input impedance
- 14:39must be no less than
- 14:4010 kilo ohms okay so therefore our
- 14:43minimum requirement is 10 kilo ohms
- 14:46to avoid loading the given signal source
- 14:49okay so the signal level will be
- 14:52sufficiently high
- 14:53to the thermal resistance noise and the
- 14:56bias current effects are
- 14:58not felt to be a critical problem
- 15:00provided that the resistance
- 15:02values less than 500 kilo ohms are used
- 15:05so therefore we are given a very broad
- 15:08range of our resistances that we can
- 15:11actually
- 15:12make use of okay so it just says here
- 15:15that
- 15:15it must not be less than 10k okay
- 15:18or it it must not be greater than 500k
- 15:22okay so but as long as it is within the
- 15:24range your design is
- 15:27is correct okay so you don't have to
- 15:30worry
- 15:30as long as you can comply with the
- 15:33requirements okay
- 15:35so this is an example this is just one
- 15:37example
- 15:38of the design for that specific problem
- 15:42because our um
- 15:46because our um requirement there
- 15:49is uh you have to have a gain
- 15:52equivalent to negative 10 so since there
- 15:55is a negative
- 15:56already in our requirement so we already
- 16:00know that you are going to make use of
- 16:02an inverting amplifier
- 16:03because if you have an inverting
- 16:05amplifier automatically you get the
- 16:07negative
- 16:08gain there okay so the only problem is
- 16:10what combination of rf and ri
- 16:12are you going to make use of so that you
- 16:15can have a value which is equivalent to
- 16:1710 okay so our um
- 16:21our formula for the voltage gain for
- 16:24your
- 16:24inverting amplifier is equivalent to
- 16:27negative rf all over r1
- 16:30so you must must use a value of rf up
- 16:35and r1 in such a way that if we divide
- 16:38them
- 16:38your answer will be equivalent to 10 so
- 16:41in this case
- 16:42it make use of 220 kilo ohms
- 16:46all over um 22
- 16:49kilo ohms so automatically we have the
- 16:52negative sign there so 220 divided by
- 16:55um 22 kilo ohms so that will give us
- 16:58again which is equivalent to
- 17:00negative 10 which is your required
- 17:04gain in the in the problem in your
- 17:07design problem
- 17:08okay so the 20 kilo ohms there okay
- 17:11where did it came from
- 17:12so the 20 kilo ohms there is your um
- 17:15compensating resistance
- 17:17and your compensating resistance is just
- 17:19the
- 17:20parallel combination of your rf which is
- 17:23220 kilo ohms
- 17:25parallel your 22 kilo ohms here
- 17:28okay so if you solve for that so that is
- 17:31220 k
- 17:33times 22 k divided by
- 17:36220 k plus 22 k
- 17:41so that will give you an exact value of
- 17:4420
- 17:45kilo ohms so luckily um these are all
- 17:48available
- 17:49so if we're going to look back
- 17:54okay so if we're going to look back at
- 17:57our resistor values where is that
- 18:00so this is your value 20 220 kilo ohms
- 18:04and make use of
- 18:0522 kilo ohms actually we can make use of
- 18:09where from from this 22 up to 51 here
- 18:14okay so we cannot uh we can uh
- 18:17we can also use this one so we can use
- 18:19100 kilo ohms divided by 10k
- 18:22okay so this is included in our
- 18:27uh in in uh this is included in our um
- 18:30option okay so you can also make
- 18:32yourself 150 kilo ohms
- 18:34and 15 kilo ohms for your r1 so that can
- 18:37still give you a gain equivalent to 10
- 18:40so you can make use of um 470 kilo ohms
- 18:43and 47 kilo ohms
- 18:45that will still give you a gain which is
- 18:47equivalent to negative 10
- 18:49okay but can we use the 56 here so if we
- 18:52make use of the 56 here
- 18:54you can have um 560 kilo ohms for your
- 18:59rf and 56 kilo ohms for your
- 19:01r1 however it says in the problem that
- 19:04we must not exceed 500 kilo ohms
- 19:08okay so therefore we are only permitted
- 19:10to use
- 19:11up to 47 470 kilo ohms and 47 ohms okay
- 19:16so
- 19:16so in a design type of a problem class
- 19:20you can have several answers okay so you
- 19:23can have several
- 19:24answers as long as you follow all of the
- 19:27conditions
- 19:28okay that is asked in the design problem
- 19:31so no problem so
- 19:33there is no such thing as a wrong design
- 19:35as long as you follow
- 19:37all the specific conditions okay
- 19:41so we have here um using the standard
- 19:44one percent resistance value
- 19:46design of vcvs non-inverting okay so
- 19:50what do we mean by non-inverting
- 19:51amplifier so in this case
- 19:53we have to place your input at the
- 19:56non-inverting terminal okay
- 19:58so to provide a voltage gain of 18 so
- 20:01remember
- 20:02that for uh for a
- 20:05non-inverting amplifier your gain
- 20:08okay so your voltage gain is equal to rf
- 20:11all over r1 plus one so we need to get
- 20:16a combination okay so you have to have a
- 20:19combination
- 20:21where in your rf all over r1
- 20:25must be equivalent to 17 okay so that if
- 20:29we add them
- 20:30your resulting gain is 18 and the
- 20:33positive answer there
- 20:35or the positive gain there will be um
- 20:38will be
- 20:39uh what you call this uh
- 20:44will be possible if we make use of a
- 20:46non-inverting because the gain for a
- 20:48non-inverting amplifier is
- 20:50positive okay so in this case we have an
- 20:53example
- 20:54so we have here um two kilo ohms we have
- 20:5734 kilo ohms and we have here
- 20:59uh 1870 ohms okay
- 21:02so if we divide 34 kilo ohms by
- 21:062 so we will be having 17 uh
- 21:09for that okay then 17.
- 21:12so we have here um uh
- 21:1634 kilo ohms divided by 2 kilo ohms so
- 21:19that will give you 17 plus one so that
- 21:22will be
- 21:23equivalent to
- 21:27so that will be equivalent to 18
- 21:30okay and then for the compensating
- 21:33resistance all we have to do is to
- 21:35um uh get the parallel combination of
- 21:38two and 34 okay which is eighteen
- 21:41thousand one thousand eight hundred
- 21:43seven ohms okay so if we're going to
- 21:46look at those values here
- 21:48so we have um 34 kilo ohms so where is
- 21:50your 34 kilo ohms
- 21:52so this is your 34
- 21:55kilo ohms so where is your 34 kilo ohms
- 21:59this one so 340 so this is 34
- 22:03and this is sure 2 kilo ohms so we're
- 22:06sure 2 kilo ohms
- 22:07here 200 and then we have the 1
- 22:11okay so we have one eight seventy
- 22:16one eight seventy so we have a one eight
- 22:20seventy so luckily we have all
- 22:22but uh when you get the parallel
- 22:25combination and you didn't get any exact
- 22:27value
- 22:28it's okay all you have to do is to
- 22:32get the one with the nearest value so
- 22:35you can have any other answer okay so
- 22:37you can
- 22:37you can uh look at this value and then
- 22:40as long as it will give you a gain of 18
- 22:42that means you will have a ratio which
- 22:44is equal to 17
- 22:46therefore your answer is correct okay
- 22:49so our non-inverting amplifier is the
- 22:53counter part of your common base
- 22:55configuration
- 22:56for our um bjt amplifiers or the
- 23:00common um source also common gate
- 23:03configurations for
- 23:05for fat okay and then the inverting
- 23:07amplifiers
- 23:10okay is the common emitter configuration
- 23:14for bjt
- 23:15or the common uh common source
- 23:19configuration for
- 23:20four okay so we have another
- 23:24type of application so we're in we call
- 23:27this
- 23:27as your voltage follower or unity
- 23:30follower
- 23:31okay so voltage follower or unity
- 23:33follower provides
- 23:34gain of unity without any phase reversal
- 23:38so what is your output what is your
- 23:41input that will also be your output
- 23:43okay so um
- 23:46this is your spool as a buffer or
- 23:49isolation amplifier
- 23:51because it allows input voltage to be
- 23:53transferred as output voltage
- 23:56while at the same time preventing load
- 23:58resistance from loading down the input
- 24:00source
- 24:01okay so in your logic circuits if you
- 24:03have this is
- 24:04the the opposite of an inverter so an
- 24:07inverter will give you the same output
- 24:10amplitude
- 24:11okay or magnitude but with a phase
- 24:13reversal
- 24:14okay so if our input for example is
- 24:16negative one your output is positive one
- 24:19so for voltage follower or unity
- 24:21followers so it is a buffer okay so
- 24:24when you see block diagrams having a
- 24:26buffer so you can make use of an
- 24:28operational amplifier for that
- 24:31so if our input is one millivolt your
- 24:34output is also
- 24:35one millivolt okay so this is just being
- 24:38used for
- 24:39electrical isolation purposes okay
- 24:42so how do we how do we connect
- 24:44operational amplifiers in such a way
- 24:47that it will be uh functioning as a
- 24:51voltage follower or a unity follower
- 24:53so this is your
- 24:56this is your connection okay all we have
- 24:59to do
- 25:00is to place an input at the in
- 25:02non-inverting terminal because
- 25:04uh we have to have the same phase
- 25:06reversal so
- 25:07our input must be placed in the input
- 25:09terminal and then this is our
- 25:12output okay so you just have to place a
- 25:14ground
- 25:15between your your inverting terminal
- 25:18and your output for your feedback
- 25:22so it is just like um
- 25:26so it is just like that um for example
- 25:30our input here is um
- 25:34so for example we have here your upper
- 25:37operational amplifier so let us call
- 25:40this your va
- 25:41okay and then let us call this your
- 25:44vb where in your vb this is your
- 25:47non-inverting side
- 25:50so this is your input voltage okay
- 25:53um this is your
- 25:57feedback here and we have here your
- 26:00output
- 26:01okay so always remember that if we if we
- 26:04make use of this configuration
- 26:06uh your ri okay so your r
- 26:09i is infinite okay so we don't have any
- 26:13input here we don't have any input
- 26:15resistance
- 26:16so this is infinite and our feedback
- 26:19resistance
- 26:19is what this is shorted so this is
- 26:22equivalent to
- 26:24to zero okay so in this case we can say
- 26:27that your va
- 26:29um is equal to your
- 26:32v out okay so if you are going to
- 26:35remember
- 26:36our voltage here virtual ground so the
- 26:39difference between va and vb here must
- 26:41be equal to
- 26:42zero so to do that our va
- 26:46must be equal to
- 26:49our va must be equal to to vb
- 26:52okay so but our vb is
- 26:55equal to your input voltage okay which
- 26:58is your
- 26:59v in but your vb is equal to your v
- 27:02in okay so your vb is equal to your ven
- 27:06and your vb is equal to va so that is
- 27:09your v in is equal to
- 27:11your v out
- 27:15so in solving for the voltage gain okay
- 27:17so your voltage gain is v
- 27:20out all over v in and since they are
- 27:22equal your voltage gain is equal to
- 27:25one okay so if you wanted a buffer
- 27:28circuit so
- 27:28in our communication subject we can see
- 27:31block diagrams having buffers circuits
- 27:34in their blocks
- 27:35so one option is to make use of an
- 27:37operational
- 27:38amplifier okay so what is its
- 27:41corresponding counterpart for bjt
- 27:44so this is just like your emitter
- 27:47follower or
- 27:48our common collector configuration
- 27:50because in our common collector
- 27:51configuration or our ammeter
- 27:54configuration this is that is in
- 27:55phase and no voltage gain or your v out
- 27:58is all
- 27:59approximately equal to your to your v
- 28:02in or for fat it is equivalent to your
- 28:05common drain
- 28:06configuration okay so that is the
- 28:10that is the third practical application
- 28:13of your op-amp so you just get your op
- 28:15amp
- 28:15you place an input okay so you put an
- 28:18input voltage at the
- 28:20non-inverting terminal and then you
- 28:22place a wire
- 28:23okay shorting your inverting terminal
- 28:25and your output here
- 28:27um you can have your inverter with you
- 28:30okay so we can place some resistors here
- 28:33so these resistors here are for
- 28:35compensating resistors only okay but
- 28:39anyways it will give you the same
- 28:42um expected output okay
- 28:48so another practical application for our
- 28:52operational application
- 28:54amplifier is other or summer
- 28:57okay so what is other or summer
- 29:01okay we have here um this provides an
- 29:04output voltage
- 29:05proportional to or equal to the
- 29:07algebraic sum
- 29:08of two or more input voltages okay
- 29:12each multiplied by a constant gain
- 29:14factor
- 29:15so this is um basically similar to a
- 29:18scalar
- 29:19except that it has more than one input
- 29:21okay so
- 29:22for example this is our um circuit for
- 29:26an adder or a summer so you will make
- 29:28usually of a
- 29:29com inverting amplifier but instead of
- 29:32having just
- 29:33one input we have several inputs okay
- 29:36and then
- 29:36our sum is the thus our
- 29:40output rather is the sum of all the
- 29:42input voltages here
- 29:44multiplied by a certain factor
- 29:47okay so how do we uh how do we evaluate
- 29:51this type of
- 29:53it
- 29:57okay so for this type of circuit
- 30:04okay so let's just say um we have
- 30:08several currents that will pass through
- 30:11your
- 30:11operational amplifier okay so those
- 30:14currents uh will can be added up
- 30:18using um the total current which is your
- 30:20i1
- 30:22plus your i2 plus your i3 here
- 30:25okay so we have here but what is your
- 30:28i1 okay so our i1 here is equivalent to
- 30:32um
- 30:33your your input voltage v1 at that
- 30:36terminal
- 30:37okay divided by your certain resistance
- 30:39r1
- 30:40okay and then we have here your i2 but
- 30:43what is your i2 there
- 30:44so that is equivalent to the voltage
- 30:46that is being applied across the
- 30:48terminal
- 30:50divided by your r2 and then what is your
- 30:53i3 so the voltage across the terminal
- 30:55which is your v3 divided by your
- 30:58your your r3 here okay so that is our
- 31:02answer okay so if you're going to
- 31:04remember what is our v
- 31:06out okay for a non for an inverting
- 31:09amplifier because that configuration is
- 31:11an
- 31:11inverting amplifier because we place all
- 31:13the inputs
- 31:14at the n at the inverting terminal so
- 31:17that will give us
- 31:18minus rf all over r1
- 31:22multiplied by our input
- 31:25voltage so that is your output voltage
- 31:29so if we combine them okay so if we
- 31:31combine them
- 31:32we can have your total output voltage
- 31:35which is equivalent to minus okay
- 31:40that is your rf since rf feedback
- 31:42resistance is common
- 31:44to all of your inputs so your rf there
- 31:47will be so your rf there
- 31:51is equivalent to sorry rf all over r1
- 31:56multiplied by your input which is your
- 31:58v1 we have here plus
- 32:00okay rf all over r2 plus
- 32:03multiplied by your v2 you have here plus
- 32:07rf all over r3 multiplied by
- 32:10v3 here okay so that
- 32:14is depending on the value of your r1
- 32:17okay but you have the same
- 32:21but you have the same rf and r1
- 32:24okay so if we wanted to simplify
- 32:28okay so if we wanted to simplify your
- 32:31circuit
- 32:32where in each of the value of r are
- 32:35equal
- 32:36okay so let us say your r1 is equal to
- 32:39your
- 32:40r2 that is equal to your r3 and that is
- 32:43equal to your
- 32:44rf we can simplify this further by
- 32:47having minus
- 32:48okay r let us just call that r
- 32:52all over r multiplied by
- 32:56v1 okay so we have here your
- 33:00um r all over r
- 33:03multiplied by v2 plus let's say
- 33:06um you have here
- 33:10um r all over r multiplied by
- 33:13v three okay since our r is constant
- 33:16we can put it outside and that is r over
- 33:19r so this is constant which is
- 33:20equivalent to one
- 33:22so that will give you a v1
- 33:25plus v2 plus v3 which is our
- 33:29output voltage okay so
- 33:32as we can see what did we have here so
- 33:35we have
- 33:36a sum of all the input
- 33:39voltages so v1 plus v2 plus v3
- 33:42so this is your other okay so usually
- 33:47in practical applications we have here
- 33:50your mixers for example
- 33:52so you you have your mixers for in for
- 33:54example you have in up in uh
- 33:56you you wanted to have a microphone and
- 33:58then you wanted to have a guitar for
- 34:01example or a piano for example and you
- 34:03wanted to blend
- 34:04the music or you wanted to amplify the
- 34:08the microphone further so you can hear
- 34:10the voice
- 34:11compared with the with the auxiliary
- 34:14input for example
- 34:15so you can make use of a uh other or a
- 34:18summing
- 34:19amplifier okay so this is your
- 34:22application for adding or summer
- 34:26okay so this is if simple addition or
- 34:29inversion is
- 34:30desired okay so you're compensating
- 34:32resistance here is
- 34:34still equivalent to the
- 34:37to the parallel combination of all the
- 34:40resistors that you can find
- 34:42in the circuit okay so that is the
- 34:45definition for your compensating
- 34:48resistance okay so what are
- 34:52an example okay let's have an example
- 34:57so we have here um in a certain
- 34:59application
- 35:00it is desired to combine two signals v1
- 35:03and v2
- 35:04to form a signal vo according to the
- 35:07following combination
- 35:08so your vo must be equivalent to
- 35:11negative v1
- 35:12minus 10 v2 okay so
- 35:16the minimum the minimum um
- 35:19input impedance for both inputs should
- 35:22no less than 10k
- 35:23so design a circuit to met to to meet
- 35:27the
- 35:29to meet the requirements okay so how are
- 35:32we going to
- 35:33solve for that
- 35:38so how are you going to solve for that
- 35:40so actually class
- 35:42we have here your answer okay so you
- 35:45have two inputs
- 35:46okay so we just have to make sure
- 35:53so we just have to make sure that
- 36:06okay so we just have to make sure that
- 36:09we can
- 36:10have this output so vo
- 36:13must be equivalent to negative v1 minus
- 36:1610
- 36:17v2 okay so since you share
- 36:22the same rf okay so we have to make sure
- 36:25that your v1
- 36:27will have a gain which is equal to 1
- 36:30so that is equivalent to 100
- 36:34divided by 100 so that is equivalent to
- 36:361
- 36:38so this is negative okay so we have here
- 36:41um
- 36:43um 100 kilo ohms divided by 100 kilo
- 36:48ohms so this will give you a gain which
- 36:49is equivalent to one
- 36:51times v1 and then you have to
- 36:54uh choose a value that when you divide
- 36:57it by 100
- 36:58the answer will become 10. okay so that
- 37:02is 100 kilo ohms here divided by 10k so
- 37:06this
- 37:06ratio here will give us a value which is
- 37:09equivalent to 10
- 37:11multiplied by our v2 so in this case
- 37:16so that will give you minus v1 plus
- 37:1910 v2
- 37:25so that is your
- 37:29design considerations
- 37:32okay so if you might be wondering um can
- 37:36i choose 200 here
- 37:37yes but you have to use 200 here
- 37:41okay and if you choose 200 here you have
- 37:43to use
- 37:4420 here okay as long as you can have
- 37:47your uh you can have the required
- 37:51design um
- 37:54problem
- 38:00okay so you have many options okay so
- 38:03you have many options
- 38:04now what is your
- 38:07rc there okay so where did the
- 38:118.33 kilo ohms came from so that is just
- 38:14your
- 38:16um
- 38:19parallel 100k parallel 10 kilo ohms
- 38:23so all the resistors that you can see
- 38:26there in your sig
- 38:27in your circuit that will be the
- 38:30that will be or that will cover your
- 38:33compensating
- 38:34resistance okay so i have here
- 38:38a problem and that will serve as your
- 38:41activity okay so it says here in a
- 38:46certain signal processing system
- 38:48okay it is necessary to combine and
- 38:51modify the levels of three signals v1 v2
- 38:54and v3
- 38:55so the desired vo is 2v1 plus
- 38:585v2 minus 10 v3
- 39:01okay so um what we need
- 39:05is a non-inverting output
- 39:09okay since this is positive but uh
- 39:12it says here that you can make use of
- 39:15linear combination circuits and or
- 39:18inverting amplifiers only
- 39:20okay so you might be wondering ah this
- 39:23is positive
- 39:24so i will be using a non-inverting
- 39:26amplifier so that i can have a positive
- 39:28answer
- 39:30but it says in the problem that you are
- 39:33to use
- 39:33only inverting amplifiers okay um
- 39:37and also so i need a positive output so
- 39:41if that is an inverting i will be
- 39:42placing a negative
- 39:44input okay but it also says here that
- 39:47you are not to use okay so do not use
- 39:50negative voltages
- 39:51as input so you have to use only
- 39:53positive
- 39:54input so you have to design okay so you
- 39:58have to design
- 40:00using inverting amplifiers okay so in
- 40:03the design
- 40:04no nothing is wrong as long as you can
- 40:07get
- 40:08this output voltage okay but you have to
- 40:11take into considerations that you will
- 40:12be using inverting amplifiers on
- 40:15also only but you can have more more
- 40:18than one
- 40:19okay and you have to make use of
- 40:21positive inputs only okay
- 40:24so this is your uh task okay and
- 40:27i want you to answer this uh
- 40:31using our um using what you have learned
- 40:35from our
- 40:36discussion okay so this is one
- 40:39application okay so this is one
- 40:42application for
- 40:43our operational amplifier okay
- 40:46so it can be used as a positive scalar
- 40:49it can be used as a
- 40:50negative scalar it can be used as a um
- 40:54unity gain okay or a buffer and then it
- 40:57can be used as a summing amplifier
- 40:59okay and then what will be our next
- 41:04so our next is if it can add likewise it
- 41:08can also
- 41:08subtract okay so if can if it can add
- 41:12it can also subtract okay so what are we
- 41:15going to make use of where are we going
- 41:18to place the input
- 41:19so that we can
- 41:22uh we can have your your
- 41:25operational amplifier work as a
- 41:28subtractor
- 41:30okay so um a subtractor or a closed-loop
- 41:33differential amplifier is used to
- 41:36provide an output proportional to or
- 41:38equal to the difference okay subtractor
- 41:40to the difference of two input signals
- 41:42so this time your inputs are supplied
- 41:45both at the inverting and the
- 41:47non-inverting terminals okay so
- 41:49for summing amplifiers all of your
- 41:52inputs are being placed only at the nun
- 41:54at the inverting terminal so if we
- 41:56wanted to make use of your op
- 41:58amp as a subtractor therefore we have to
- 42:01place an input
- 42:02both to your inverting and to your
- 42:04non-inverting terminal so how does this
- 42:07look like
- 42:08okay so this is your subtractor
- 42:11okay so you have an input
- 42:14so if you have a non-inverting amplifier
- 42:18this v1 here is grounded if you have an
- 42:21inverting amplifier this v2 here
- 42:24is grounded okay if you have a summing
- 42:27amplifier
- 42:28um all of the inputs v1 and v2 are being
- 42:31placed at the
- 42:32inverting terminal if you have a buffer
- 42:35okay
- 42:35our input is in this one and then we
- 42:37just have to place a wire between the
- 42:39inverting and the
- 42:41output terminal okay so for a subtractor
- 42:44we need to place an input both at the
- 42:46inverting terminal and the non-inverting
- 42:48terminal
- 42:49okay so how do we arrive with this
- 42:53uh v2 minus v1 here okay so
- 42:58if you're going to remember from your um
- 43:01from your circuit analysis okay so we
- 43:04have what we call the superposition
- 43:06theorem
- 43:07so what does the superposition theorem
- 43:11um function so how does the super
- 43:15positions during functions so we're just
- 43:17going to work on only one
- 43:20input terminal at a time okay so that
- 43:22means
- 43:23when we are dealing with the with your
- 43:25v1
- 43:26so we are going to uh place your v2
- 43:29grounded
- 43:30and at the same time when we're dealing
- 43:32with veto already
- 43:33we are going to ground your v1 okay so
- 43:36let us start first with v1
- 43:40so when we are working on v1 okay so
- 43:43that means your v2
- 43:44is grounded so when your v2 is grounded
- 43:48okay so when your v2 is grounded it's
- 43:50just like you're working on
- 43:52as as an inverting amplifier
- 43:56so when you are working as an inverting
- 43:58amplifier
- 43:59okay so v1 is acting alone
- 44:03so that is an inverting amplifier so
- 44:05that will give
- 44:06us an output so let us call that output
- 44:09as v01
- 44:10okay so your output is a non in
- 44:13is an inverting amplifier and that is
- 44:15equivalent to rf
- 44:17all over r1 multiplied by your
- 44:20v1 okay so this is just like an
- 44:23inverting amplifier
- 44:28so this is just like an inverting
- 44:30amplifier
- 44:32okay so what if v2 acts alone
- 44:36so that means we are going to ground
- 44:38your v1 so if we ground your b1 v1
- 44:41it is just like working as a
- 44:43non-inverting
- 44:46amplifier so when you have a
- 44:50non-inverting amplifier
- 44:51okay let us call this vo2
- 44:55let us call this vo2 and that will give
- 44:58you rf
- 44:58all over r1 plus 1 okay multiplied by
- 45:03v2 okay so for superposition through
- 45:07them up uh
- 45:08upon getting the individual answers
- 45:12we are going to combine them so we're
- 45:14going to either add them or subtract
- 45:16them
- 45:16but since this is of negative sign so if
- 45:18we add them
- 45:19we will be having a negative sign here
- 45:22okay so for simplification
- 45:24for a simplification purposes we can
- 45:27just assume that your rf
- 45:28plus r1 rf all over r1 plus 1 is
- 45:32approximately equal to rf all over r1
- 45:35okay so combining the two so we have
- 45:37your v out
- 45:38and your v out is equivalent to vo2
- 45:42minus vo1 okay because of the negative
- 45:46sign there
- 45:47okay or plus so vo2 is um rf
- 45:51all over r1 times v2 plus
- 45:54okay minus but that's a negative sign so
- 45:56we have rf
- 45:57all over r1 multiplied by v1
- 46:00okay so factoring out your rf all over
- 46:03r1
- 46:04we have here an answer which is
- 46:06equivalent to v2
- 46:08minus v1 okay so if we are going to
- 46:14if we are going to simplify this further
- 46:18and let us say rf will be equal to r1
- 46:21so we will be getting an output which is
- 46:23the difference
- 46:25okay so we will be getting an output
- 46:27which is the difference between your two
- 46:29input voltage
- 46:30which is your v2 minus v1 so we have
- 46:34a subtractor okay so that is
- 46:37how your operational amplifier can be
- 46:41um can be applied as
- 46:44an as a subtractor so as you can see
- 46:48i'm just changing where are you going to
- 46:51place your
- 46:52input you have several applications
- 46:56for your operational amplifier so that
- 46:58means your operational amplifier class
- 47:00is very versatile
- 47:02okay and it can add it can subtract
- 47:06okay so actually it was called
- 47:08operational amplifiers
- 47:09because it it was really designed it was
- 47:12really first designed
- 47:14to um to perform
- 47:17mathematical operations that's why it
- 47:19was called operational
- 47:21amplifiers okay so this is a very simple
- 47:24type of a subtractor
- 47:26however in practical use in practical
- 47:30use
- 47:30we have here your practical application
- 47:34for a
- 47:35subtractor okay so this is
- 47:38what we call this is how we uh
- 47:43this is how we design or how we use your
- 47:47um uh
- 47:51actual subtractor class okay so where it
- 47:53we have four
- 47:54resistors here okay so this is like a
- 47:58voltage divider for your v1
- 48:00and your v2 okay so for example um
- 48:04we have here your v2 alone for example
- 48:07uh if we ground your v1 here so it is
- 48:09working as an uh
- 48:11as a non-inverting amplifier so we can
- 48:14get your
- 48:15first output which is minus r4 which is
- 48:18your feedback
- 48:19all over r3 multiplied by our
- 48:24v2 here okay and if your v1
- 48:27is acting alone and your v2 is grounded
- 48:30okay so the input voltage will be
- 48:34uh so the input v1 here will be divided
- 48:37between
- 48:38r1 and r2 and the input is the voltage
- 48:41across your r2
- 48:42because this will serve as a uh voltage
- 48:45divider
- 48:46okay so for vo2
- 48:50okay so let us call that vo2 so that is
- 48:53a non-inverting amplifier so we have one
- 48:56plus
- 48:56r4 all over r3 okay
- 49:00um by the input voltage but what is the
- 49:04input voltage so the input voltage is
- 49:06the voltage across r2
- 49:08so we have a voltage divider between r1
- 49:11and r2 multiplied by our
- 49:14v1 here okay so that is your
- 49:19that is your v2 so to get the total
- 49:22value so to get the total output voltage
- 49:26so that is a combination of your um
- 49:30r3 1
- 49:33plus r4 all over r3 multiplied by
- 49:37r2 all over r1 plus r2
- 49:40multiplied by v1 so minus
- 49:44you have here r4 all over r3 multiplied
- 49:47by
- 49:49by v2 okay so just what we did earlier
- 49:53this time we just have your voltage
- 49:55divider configuration here
- 49:57okay so for instrumentation purposes we
- 50:00make use of
- 50:01the balance closed loop differential
- 50:03amplifier
- 50:04so the balance closed loop differential
- 50:07amplifier is the most important case of
- 50:09closed loop differential amplifier
- 50:11so it is said to be balanced if we get
- 50:14if we make use of these values
- 50:16so your r here species specifies a
- 50:20certain
- 50:21value that are equal okay and
- 50:24this a here specifies again
- 50:28okay so uh the two gains are equal
- 50:31and opposite so how are we going to
- 50:34attain this balance
- 50:35close loop differential amplifier if
- 50:38we're going to follow this
- 50:40suggested values for r1 r2 r3 and
- 50:43r4 okay so if we're going to um
- 50:48if we're going to
- 50:51substitute this value in our equation
- 50:55here
- 50:56so if we're going to substitute those
- 50:57values in our equation
- 50:59so that will give us okay so your v out
- 51:02is equal to 1 plus what is supposed to
- 51:05be the value of
- 51:06r4 r4 is equivalent to a
- 51:09r3 or let us call that ar divided by
- 51:12r3 which is equivalent to r okay and
- 51:15this is equivalent to what is our r2
- 51:18r2 is equivalent to ar all over
- 51:21r1 is equal to r plus r2 is equivalent
- 51:25to
- 51:26ar okay multiplied by v1
- 51:29so this is r4 r4 is equivalent to
- 51:32a r
- 51:36ar all over r multiplied by v2
- 51:40okay so we have here um a
- 51:43r here will be cancelled out so i have
- 51:46here 1 plus
- 51:47a and then i have here a r
- 51:50i can factor out your r here so this is
- 51:53equivalent to 1
- 51:54plus a okay so i can cancel out your
- 51:58r here and i can cancel out your 1 over
- 52:01a
- 52:01i here so i have a remaining a there for
- 52:04my
- 52:04v1 minus i can cancel out your r there i
- 52:08have here
- 52:09a multiplied by your v2 okay so your a
- 52:13can be factored out so this is simply v1
- 52:16minus v2 so our v out for a balanced
- 52:20amplifier is simply the difference
- 52:24okay so that is simply the difference
- 52:28between v1 and v2
- 52:31multiplied by a certain gain but you
- 52:35have to make sure
- 52:36okay but you have to make sure that you
- 52:38follow
- 52:39this specific resistor requirement
- 52:43okay so this is the derivation
- 52:50so we have here an example a circuit is
- 52:52desired for an
- 52:53instrumentation application in which the
- 52:56difference between two signals p1 and v2
- 52:59is to be amplified by a factor of 10 so
- 53:02that
- 53:02is 10 v1 minus v2 design a circuit to
- 53:06perform the required function
- 53:08so the required function is that your a
- 53:16so your a is equivalent to 10
- 53:19okay so so we have to choose a value for
- 53:23r okay which are similar to every values
- 53:27of
- 53:27our four resistors that is in our
- 53:29circuit
- 53:30having a resistance which is equal to 10
- 53:33okay sorry again which is equal to 10 so
- 53:36what is our
- 53:37um answer for that so we can make use of
- 53:41this one okay
- 53:42so in this case your r3
- 53:46is equal to r okay and your r4 is equal
- 53:50to ar
- 53:51our gain is 10 okay so 10 times 10
- 53:55so we have here 10 100 kilo ohms so our
- 53:58r1 is equal to r so let's say this is 10
- 54:01kilo ohms
- 54:02and then this is equal to 10 times r
- 54:05which is equivalent to 100 kilos
- 54:07so can we make use of 20 yes we can make
- 54:10use of 20. so this is 20k
- 54:13this is 200k so this is 20k this is 200k
- 54:17so we can make use of 30. so this is 30k
- 54:20this is 300k this is
- 54:2210 30k this is 300 kilos so that is
- 54:25what uh uh balance close
- 54:29loop differential amplifier operates
- 54:32okay
- 54:32so don't forget the don't don't be
- 54:36confused with the circuit because the
- 54:38circuit is just the same
- 54:40so when you say this sign all you have
- 54:42to do is to change
- 54:44the value of your resistances
- 54:47okay so there are more upper
- 54:50mathematical operation so what else can
- 54:53uh can
- 54:54an operational amplifier do so aside
- 54:56from subtracting aside from adding aside
- 54:58from inverting aside from multiplying
- 55:01okay so it can also integrate it can
- 55:04also differentiate and it can also
- 55:06compare
- 55:07so we have an integrator differentiator
- 55:10and
- 55:10comparator and i will be discussing that
- 55:13on the next
- 55:14video okay so that's it for now
- 55:17okay so i will be ending our discussion
- 55:20here and wait for the second
- 55:22uh the follow-up video for the other
- 55:24practical applications of
- 55:26our operational amplifiers okay so thank
- 55:29you very much and don't forget to hit
- 55:31the like button
- 55:32after watching okay thank you and god
- 55:39bless
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This page contains the full transcript of OP AMP Application Part 1 (Electronics 2) by Engr. Kat, generated from the public captions YouTube serves with the video. The transcript has 7,545 words across 1,299 segments, with the original timestamps preserved so you can click any line to jump to that moment in the embedded player.
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Use the transcript to take notes, quote the speaker, build a study guide, generate a summary with ChatGPT or Claude via the YouTube Summary tool, or export it as a timed subtitle file with YouTube to SRT. You can also re-open it in the transcriber to choose a caption track available on the video.
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