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Program Studi Teknik Elektro Konsentrasi Mekatronika
Universitas Katolik Parahyangan
DASAR RANGKAIAN LISTRIK
Ali Sadiyoko, S.T., M.T.
Faisal Wahab, S.Pd., M.T.
FAKULTAS TEKNOLOGI INDUSTRI
PROGRAM STUDI
TEKNIK ELEKTRO KONSENTRASI MEKATRONIKA
2016
Program Studi Teknik Elektro Konsentrasi Mekatronika
Universitas Katolik Parahyangan
Topik 5
Operational Amplifier
β€’ Gelombang Sinusoidal
β€’ Pengantar
β€’ Ideal Op-Amp
β€’ Inverter Op-Amp
β€’ Non-Inverter Op-Amp
β€’ Summing Op-Amp
β€’ Diferensial Op-Amp
β€’ Cascade Op-Amp
Program Studi Teknik Elektro Konsentrasi Mekatronika
Universitas Katolik Parahyangan
Gelombang Sinusoidal
Dimana :
A = Amplituda
πœ” = 2πœ‹π‘“ = π‘“π‘Ÿπ‘’π‘˜π‘’π‘’π‘›π‘ π‘– 𝑠𝑒𝑑𝑒𝑑
𝑓 =
1
𝑇
= π‘“π‘Ÿπ‘’π‘˜π‘’π‘’π‘›π‘ π‘–
𝑑 = π‘ π‘Žπ‘‘π‘’π‘Žπ‘› π‘‘π‘’π‘‘π‘–π‘˜
T
A
πœ‹
πœ” 𝑑2πœ‹πœ‹
2
3πœ‹
2
)
2
(sin t
T
Ay

ο€½
)(sin tAy 
)2(sin tfAy 
A
Program Studi Teknik Elektro Konsentrasi Mekatronika
Universitas Katolik Parahyangan
Gambarkan Sinyal sinusoidal y= 2 sin (6280t)
Jawab :
Amplitudo
A = 2
perioda
πœ” =
2πœ‹
𝑇
𝑇 =
2πœ‹
πœ”
=
2π‘₯3,14
6280
= 0.001 𝑠
frekuensi
πœ” = 2πœ‹π‘“
𝑓 =
πœ”
2πœ‹
=
6280
2π‘₯3.14
= 1000 𝐻𝑧/1π‘˜π»π‘§
Program Studi Teknik Elektro Konsentrasi Mekatronika
Universitas Katolik Parahyangan
Gain
(A)
𝑉𝑠
𝑅 𝑠
𝑉𝑙
+
βˆ’
Op-Amp
𝑽𝒍 = 𝑨𝑽 𝒔
Tegangan output 𝑉𝑙 adalah penguatan dari Tegangan sumber 𝑉𝑠
Amplifier LoadSource
Program Studi Teknik Elektro Konsentrasi Mekatronika
Universitas Katolik Parahyangan
+
-
𝑣𝑠
𝑅 𝑠
𝑅𝑖𝑛
𝐴 𝑣 𝑖𝑛
𝑅 π‘œπ‘’π‘‘
+
βˆ’
𝑣𝑖𝑛
𝑣𝑖𝑛 =
𝑅𝑖𝑛
𝑅 𝑠 + 𝑅𝑖𝑛
𝑣𝑠 𝑣𝑙 =
𝑅𝑙
𝑅 π‘œπ‘’π‘‘ + 𝑅𝑙
𝐴 𝑣 𝑖𝑛
+
βˆ’
𝑣𝑙
π’—π’Šπ’ = 𝒗 𝒔
Idealnya 𝒗𝒍 = 𝑨 𝒗 π’Šπ’
𝒗𝒍 = 𝑨 𝒗 𝒔
𝑅𝑙
𝑅𝑖𝑛= ∞
(open loop)
𝑅 π‘œπ‘’π‘‘ = 0
(close loop)
Program Studi Teknik Elektro Konsentrasi Mekatronika
Universitas Katolik Parahyangan
+
-
𝑅𝑖𝑛
𝐴 𝑣 𝑖𝑛
𝑅 π‘œπ‘’π‘‘
+
βˆ’
𝑣𝑖𝑛
𝑣 𝑝
𝑣 𝑛
Karakteristik Ideal Op-Amp
1. 𝑅𝑖𝑛= ∞, (open circuit)
2. 𝑅 π‘œ = 0, (short circuit)
3. 𝐴 = ∞,
𝑣 𝑝 = 𝑣 𝑛
𝑖 𝑝 = 𝑖 𝑛 = 0
𝑖 𝑝
𝑖 𝑛
Circuit Model
𝑣𝑖𝑛 = 𝑣 𝑝 βˆ’ 𝑣 𝑛
Dengan gain 𝐴 = ∞, sedangkan
𝑣𝑐𝑐 dibatasi 24 V, Maka,
𝑣 𝑐𝑐
𝐴
= 0
Pada Op-Amp ideal 𝑅𝑖𝑛= ∞ sehingga
arus yang masuk 𝑣 𝑝 dan 𝑣 𝑛 dianggap nol
𝑣 π‘œ
Program Studi Teknik Elektro Konsentrasi Mekatronika
Universitas Katolik Parahyangan
+
-
𝑣𝑠
𝑅 𝑠
𝑅𝑓
+
βˆ’
𝑣 π‘œπ‘£ 𝑝
𝑣 𝑛
Inverting
Amplifier
Circuit Model
𝑣𝑠
𝑅 𝑠
𝑅𝑓
+
βˆ’
𝑣 π‘œ
𝑣 𝑝
𝑣 𝑛
Tentukan close loop voltage
gain 𝐴 =
π‘‰π‘œ
𝑉𝑠
!
𝐴 𝑣 𝑖𝑛
+
βˆ’
𝑣𝑖𝑛
𝑅𝑖𝑛
𝑅 π‘œπ‘’π‘‘
Program Studi Teknik Elektro Konsentrasi Mekatronika
Universitas Katolik Parahyangan
+
-
Terminal non-inversi
dihubungkan ke ground,
sehingga 𝑣 𝑝 = 0 maka
𝑣 𝑝 = 𝑣 𝑛 = 0 dan
𝑣𝑠
𝑅 𝑠
𝑅𝑓
+
βˆ’
𝑣 π‘œ
𝑣 𝑝
𝑣 𝑛
𝑣𝑠 βˆ’ 𝑣 𝑛
𝑅 𝑠
βˆ’
𝑣 𝑛 βˆ’ 𝑣 π‘œ
𝑅𝑓
βˆ’ 𝑖 𝑛 = 0
𝑣𝑠 βˆ’ 𝑣 𝑛
𝑅 𝑠
=
𝑣 𝑛 βˆ’ 𝑣 π‘œ
𝑅𝑓
𝑣𝑠 𝑅𝑓 βˆ’ 𝑣 𝑛 𝑅𝑓 = 𝑣 𝑛 𝑅 𝑠 βˆ’ 𝑣 π‘œ 𝑅 𝑠
𝑣𝑠 𝑅𝑓 = 𝑣 𝑛(𝑅 𝑠 + 𝑅𝑓) βˆ’ 𝑣 π‘œ 𝑅 𝑠
karena 𝑣 𝑛 = 0
𝑣𝑠 𝑅𝑓 = βˆ’ 𝑣 π‘œ 𝑅 𝑠
𝑣 π‘œ
𝑣𝑠
= βˆ’
𝑅𝑓
𝑅 𝑠
𝐴 =
𝑣 π‘œ
𝑣𝑠
= βˆ’
𝑅𝑓
𝑅 𝑠
Tentukan close loop
voltage gain 𝐴 =
𝑣 π‘œ
𝑣 𝑠
!
Inverting
Amplifier
KCL di node 𝑣 𝑛: 𝑖1 βˆ’ 𝑖2 βˆ’ 𝑖 𝑛 = 0
𝑖 𝑝 = 𝑖 𝑛 = 0
𝑖 𝑝
𝑖 𝑛
𝐴 𝑣 𝑖𝑛
+ βˆ’
𝑖1
+ βˆ’
𝑖2
Program Studi Teknik Elektro Konsentrasi Mekatronika
Universitas Katolik Parahyangan
𝑣𝑠 = 0.5
10Ω
+
βˆ’
𝑣 π‘œπ‘£ 𝑝
𝑣 𝑛
Contoh Inverting Amplifier
25Ω
1. Tentukan 𝑣 π‘œ
2. Tentukan arus i
𝑣 π‘œ = βˆ’
𝑅𝑓
𝑅 𝑠
𝑣𝑠
𝑣 π‘œ = βˆ’
25
10
0.5
𝑣 π‘œ = βˆ’1.25
+ βˆ’
𝑖
𝑖 =
𝑣𝑖 βˆ’ 𝑣 𝑛
𝑅 𝑠
𝑖 =
0.5 βˆ’ 0
10
𝑖 = 0.05 𝐴
Program Studi Teknik Elektro Konsentrasi Mekatronika
Universitas Katolik Parahyangan
𝑣𝑠
𝑅 𝑠
𝑅𝑓
+
βˆ’
𝑣 π‘œ
𝑣 𝑝
𝑣 𝑛
Tentukan close loop voltage
gain 𝐴 =
𝑣 π‘œ
𝑣 𝑠
!
0 βˆ’ 𝑣 𝑛
𝑅 𝑠
βˆ’
𝑣 𝑛 βˆ’ 𝑣 π‘œ
𝑅𝑓
βˆ’ 𝑖 𝑛 = 0
βˆ’
𝑣 𝑛
𝑅 𝑠
=
𝑣 𝑛 βˆ’ 𝑣 π‘œ
𝑅𝑓
βˆ’π‘£π‘  𝑅𝑓 = 𝑣𝑠 𝑅 𝑠 βˆ’ 𝑣 π‘œ 𝑅 𝑠
𝑣 π‘œ
𝑣𝑠
=
𝑅𝑓 + 𝑅 𝑠
𝑅 𝑠
𝑣𝑠(𝑅𝑓 + 𝑅 𝑠) = 𝑣 π‘œ 𝑅 𝑠
Non-Inverting
Amplifier
Terminal non-inversi dihubungkan ke sumber, sehingga 𝑣 𝑝 = 𝑣𝑠 maka 𝑣 𝑝 = 𝑣 𝑛 = 𝑣𝑠
Op-amp ideal 𝑖 𝑝 = 𝑖 𝑛 = 0
βˆ’
𝑣𝑠
𝑅 𝑠
=
𝑣𝑠 βˆ’ 𝑣 π‘œ
𝑅𝑓
dan 𝑣 𝑝 = 𝑣 𝑛 = 𝑣𝑠
𝑖 𝑛
𝑖1
𝑖2
Program Studi Teknik Elektro Konsentrasi Mekatronika
Universitas Katolik Parahyangan
Tentukan close loop voltage
gain 𝐴 =
𝑣 π‘œ
𝑣 𝑠
!
0 βˆ’ 𝑣 𝑛
𝑅 𝑠
βˆ’
𝑣 𝑛 βˆ’ 𝑣 π‘œ
𝑅𝑓
βˆ’ 𝑖 𝑛 = 0
βˆ’
𝑣 𝑛
𝑅 𝑠
=
𝑣 𝑛 βˆ’ 𝑣 π‘œ
𝑅𝑓
βˆ’π‘£π‘  𝑅𝑓 = 𝑣𝑠 𝑅 𝑠 βˆ’ 𝑣 π‘œ 𝑅 𝑠
𝑣 π‘œ
𝑣𝑠
=
𝑅𝑓 + 𝑅 𝑠
𝑅 𝑠
𝑣𝑠(𝑅𝑓 + 𝑅 𝑠) = 𝑣 π‘œ 𝑅 𝑠
Non-Inverting
Amplifier
Terminal non-inversi dihubungkan ke sumber, sehingga 𝑣 𝑝 = 𝑣𝑠 maka 𝑣 𝑝 = 𝑣 𝑛 = 𝑣𝑠
Op-amp ideal 𝑖 𝑝 = 𝑖 𝑛 = 0
βˆ’
𝑣𝑠
𝑅 𝑠
=
𝑣𝑠 βˆ’ 𝑣 π‘œ
𝑅𝑓
dan 𝑣 𝑝 = 𝑣 𝑛 = 𝑣𝑠
𝑅 𝑠
𝑅𝑓
𝑣 𝑝
𝑣 𝑛
+
βˆ’
𝑣 π‘œ
Program Studi Teknik Elektro Konsentrasi Mekatronika
Universitas Katolik Parahyangan
Contoh non-Inverting Amplifier
6𝑉
4Ω
10Ω
+
βˆ’
𝑣 π‘œπ‘£ 𝑝
𝑣 𝑛
4𝑉
6 βˆ’ 𝑣 𝑛
𝑅 𝑠
βˆ’
𝑣 𝑛 βˆ’ 𝑣 π‘œ
𝑅𝑓
βˆ’ 𝑖 𝑛 = 0
Karena 𝑣 𝑝 = 𝑣 𝑛 = 𝑣𝑠 dan 𝑖 𝑝 = 𝑖 𝑛 = 0
6 βˆ’ 4
4
βˆ’
4 βˆ’ 𝑣 π‘œ
10
βˆ’ 0 = 0
6 βˆ’ 4
4
=
4 βˆ’ 𝑣 π‘œ
10
2
4
=
4 βˆ’ 𝑣 π‘œ
10
5 = 4 βˆ’ 𝑣 π‘œ
𝑣 π‘œ = βˆ’1
1. Tentukan 𝑣 π‘œ
KCL di node 𝑣 𝑛
Program Studi Teknik Elektro Konsentrasi Mekatronika
Universitas Katolik Parahyangan
𝑣𝑠
+
βˆ’
𝑣 π‘œ
𝑣 𝑝
𝑣 𝑛
Buffer
Amplifier
Terminal non-inversi (𝑣 𝑝) dihubungkan ke sumber,
sehingga 𝒗 𝒑= 𝒗 𝒏 maka 𝒗 𝒑 = 𝒗 𝒏 = 𝒗 𝒔
Dan terminal 𝑣 𝑛 terhubung langsung dengan 𝑣𝑠 𝑣 𝑛 = 𝑣𝑠
Sehingga 𝒗 𝒑 = 𝒗 𝒏 = 𝒗 𝒔 = 𝒗 𝒐
Jadi gain loop tertutupnya adalah 1.
Program Studi Teknik Elektro Konsentrasi Mekatronika
Universitas Katolik Parahyangan
Summing
Amplifier 𝑣1
𝑅1
𝑅𝑓
+
βˆ’
𝑣 π‘œπ‘£ 𝑝
𝑣 𝑛𝑣2
𝑣3
𝑅2
𝑅3
𝑖1 + 𝑖2 + 𝑖3 βˆ’ 𝑖 = 0
𝑖1
𝑖2
𝑖3
𝑖
𝑣1 βˆ’ 𝑣 𝑛
𝑅1
+
𝑣2 βˆ’ 𝑣 𝑛
𝑅2
+
𝑣3 βˆ’ 𝑣 𝑛
𝑅3
=
𝑣 𝑛 βˆ’ 𝑣 π‘œ
𝑅𝑓
𝑣1
𝑅1
+
𝑣2
𝑅2
+
𝑣3
𝑅3
=
βˆ’π‘£ π‘œ
𝑅𝑓
βˆ’
𝑅𝑓
𝑅1
𝑣1 +
𝑅𝑓
𝑅2
𝑣2 +
𝑅𝑓
𝑅3
𝑣3 = 𝑣 π‘œ
Terminal non-inversi dihubungkan ke ground,
sehingga 𝑣 𝑝 = 0 maka 𝑣 𝑝 = 𝑣 𝑛 = 0
KCL di node 𝑣 𝑛
Program Studi Teknik Elektro Konsentrasi Mekatronika
Universitas Katolik Parahyangan
2 𝑉
5Ω 10 Ω
+
βˆ’
𝑣 π‘œ
𝑣 𝑝
𝑣 𝑛
1 𝑉
2.5Ω
𝑖1
𝑖2
Contoh Summing Amplifier
2 Ω
βˆ’
10
5
2 +
10
2,5
1 = 𝑣 π‘œ
βˆ’ 4 + 4 = 𝑣 π‘œ
1. Tentukan 𝑣 π‘œ
2. Tentukan 𝑖 π‘œ
βˆ’8 = 𝑣 π‘œ
𝑖 π‘œ =
𝑣 π‘œ βˆ’ 0
10
+
𝑣 π‘œ βˆ’ 0
2
𝑖 π‘œ = βˆ’
8
10
βˆ’
8
2
𝑖 π‘œ = βˆ’0.8 βˆ’ 4
𝑖 π‘œ = βˆ’4.8 𝐴
1. Mentukan 𝑣 π‘œ
1. Mentukan 𝑖 π‘œ
𝑖0
Program Studi Teknik Elektro Konsentrasi Mekatronika
Universitas Katolik Parahyangan
Difference Amplifier
𝑉1
𝑅1
𝑅4
+
βˆ’
π‘‰π‘œπ‘‰π‘
𝑉𝑛
𝑉2
𝑅2
𝑅3
𝑖1
𝑖2
Program Studi Teknik Elektro Konsentrasi Mekatronika
Universitas Katolik Parahyangan
π‘‰π‘œ =
𝑅2 + 𝑅1
𝑅1
𝑉𝑛 βˆ’
𝑅2
𝑅1
𝑉1
karena 𝑉𝑝 = 𝑉𝑛
π‘‰π‘œ =
𝑅2 + 𝑅1
𝑅1
𝑅4
𝑅3 + 𝑅4
𝑉2 βˆ’
𝑅2
𝑅1
𝑉1
𝑉𝑝 =
𝑅4
𝑅3 + 𝑅4
𝑉2
𝑉2 βˆ’ 𝑉𝑝
𝑅3
=
𝑉𝑝
𝑅4
𝑉2 𝑅4 βˆ’ 𝑉𝑝 𝑅4 = 𝑉𝑝 𝑅3
𝑉2 𝑅4 = 𝑉𝑝 𝑅3 + 𝑉𝑝 𝑅4
𝑉2 𝑅4 = 𝑉𝑝(𝑅3 + 𝑅4)
𝑉𝑝 =
𝑅4
𝑅3 + 𝑅4
𝑉2
KCL di node 𝑣 𝑝
𝑉1 βˆ’ 𝑉𝑛
𝑅1
=
𝑉𝑛 βˆ’ π‘‰π‘œ
𝑅2
𝑉1 𝑅2 βˆ’ 𝑉𝑛 𝑅2 = 𝑉𝑛 𝑅1 βˆ’ π‘‰π‘œ 𝑅1
π‘‰π‘œ 𝑅1 = 𝑉𝑛 𝑅2 + 𝑅1 βˆ’ 𝑉1 𝑅2
π‘‰π‘œ =
𝑅2 + 𝑅1
𝑅1
𝑉𝑛 βˆ’
𝑅2
𝑅1
𝑉1
KCL di node 𝑣 𝑛
Program Studi Teknik Elektro Konsentrasi Mekatronika
Universitas Katolik Parahyangan
Cascaded Op Amp Circuits
𝑉𝑠
𝑅 𝑠
𝑅𝑓
+
βˆ’
π‘‰π‘œ
𝑉𝑝
𝑉𝑛
𝑉𝑝
𝑉𝑛
𝑅 𝑠
𝑅𝑓
𝑉𝑠
𝑅 𝑠
𝑅𝑓
+
βˆ’
π‘‰π‘œ
𝑉𝑝
𝑉𝑛
𝑉𝑝
𝑉𝑛
𝑅 𝑠
𝑅𝑓
Inverting
Amplifier
Non-Inverting
Amplifier
Program Studi Teknik Elektro Konsentrasi Mekatronika
Universitas Katolik Parahyangan
20mV
3
12
+
βˆ’
π‘‰π‘œ
𝑉𝑝
𝑉𝑛
𝑉𝑝
𝑉𝑛
4
10
Op-amp pertama Op-amp kedua
𝑣 π‘œ =
12 + 3
3
20
𝑣 π‘œ = 100π‘šπ‘‰
𝑣 π‘œ =
10 + 4
4
100
𝑣 π‘œ = 350π‘šπ‘‰

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05. operational amplifier

  • 1. Program Studi Teknik Elektro Konsentrasi Mekatronika Universitas Katolik Parahyangan DASAR RANGKAIAN LISTRIK Ali Sadiyoko, S.T., M.T. Faisal Wahab, S.Pd., M.T. FAKULTAS TEKNOLOGI INDUSTRI PROGRAM STUDI TEKNIK ELEKTRO KONSENTRASI MEKATRONIKA 2016
  • 2. Program Studi Teknik Elektro Konsentrasi Mekatronika Universitas Katolik Parahyangan Topik 5 Operational Amplifier β€’ Gelombang Sinusoidal β€’ Pengantar β€’ Ideal Op-Amp β€’ Inverter Op-Amp β€’ Non-Inverter Op-Amp β€’ Summing Op-Amp β€’ Diferensial Op-Amp β€’ Cascade Op-Amp
  • 3. Program Studi Teknik Elektro Konsentrasi Mekatronika Universitas Katolik Parahyangan Gelombang Sinusoidal Dimana : A = Amplituda πœ” = 2πœ‹π‘“ = π‘“π‘Ÿπ‘’π‘˜π‘’π‘’π‘›π‘ π‘– 𝑠𝑒𝑑𝑒𝑑 𝑓 = 1 𝑇 = π‘“π‘Ÿπ‘’π‘˜π‘’π‘’π‘›π‘ π‘– 𝑑 = π‘ π‘Žπ‘‘π‘’π‘Žπ‘› π‘‘π‘’π‘‘π‘–π‘˜ T A πœ‹ πœ” 𝑑2πœ‹πœ‹ 2 3πœ‹ 2 ) 2 (sin t T Ay  ο€½ )(sin tAy  )2(sin tfAy  A
  • 4. Program Studi Teknik Elektro Konsentrasi Mekatronika Universitas Katolik Parahyangan Gambarkan Sinyal sinusoidal y= 2 sin (6280t) Jawab : Amplitudo A = 2 perioda πœ” = 2πœ‹ 𝑇 𝑇 = 2πœ‹ πœ” = 2π‘₯3,14 6280 = 0.001 𝑠 frekuensi πœ” = 2πœ‹π‘“ 𝑓 = πœ” 2πœ‹ = 6280 2π‘₯3.14 = 1000 𝐻𝑧/1π‘˜π»π‘§
  • 5. Program Studi Teknik Elektro Konsentrasi Mekatronika Universitas Katolik Parahyangan Gain (A) 𝑉𝑠 𝑅 𝑠 𝑉𝑙 + βˆ’ Op-Amp 𝑽𝒍 = 𝑨𝑽 𝒔 Tegangan output 𝑉𝑙 adalah penguatan dari Tegangan sumber 𝑉𝑠 Amplifier LoadSource
  • 6. Program Studi Teknik Elektro Konsentrasi Mekatronika Universitas Katolik Parahyangan + - 𝑣𝑠 𝑅 𝑠 𝑅𝑖𝑛 𝐴 𝑣 𝑖𝑛 𝑅 π‘œπ‘’π‘‘ + βˆ’ 𝑣𝑖𝑛 𝑣𝑖𝑛 = 𝑅𝑖𝑛 𝑅 𝑠 + 𝑅𝑖𝑛 𝑣𝑠 𝑣𝑙 = 𝑅𝑙 𝑅 π‘œπ‘’π‘‘ + 𝑅𝑙 𝐴 𝑣 𝑖𝑛 + βˆ’ 𝑣𝑙 π’—π’Šπ’ = 𝒗 𝒔 Idealnya 𝒗𝒍 = 𝑨 𝒗 π’Šπ’ 𝒗𝒍 = 𝑨 𝒗 𝒔 𝑅𝑙 𝑅𝑖𝑛= ∞ (open loop) 𝑅 π‘œπ‘’π‘‘ = 0 (close loop)
  • 7. Program Studi Teknik Elektro Konsentrasi Mekatronika Universitas Katolik Parahyangan + - 𝑅𝑖𝑛 𝐴 𝑣 𝑖𝑛 𝑅 π‘œπ‘’π‘‘ + βˆ’ 𝑣𝑖𝑛 𝑣 𝑝 𝑣 𝑛 Karakteristik Ideal Op-Amp 1. 𝑅𝑖𝑛= ∞, (open circuit) 2. 𝑅 π‘œ = 0, (short circuit) 3. 𝐴 = ∞, 𝑣 𝑝 = 𝑣 𝑛 𝑖 𝑝 = 𝑖 𝑛 = 0 𝑖 𝑝 𝑖 𝑛 Circuit Model 𝑣𝑖𝑛 = 𝑣 𝑝 βˆ’ 𝑣 𝑛 Dengan gain 𝐴 = ∞, sedangkan 𝑣𝑐𝑐 dibatasi 24 V, Maka, 𝑣 𝑐𝑐 𝐴 = 0 Pada Op-Amp ideal 𝑅𝑖𝑛= ∞ sehingga arus yang masuk 𝑣 𝑝 dan 𝑣 𝑛 dianggap nol 𝑣 π‘œ
  • 8. Program Studi Teknik Elektro Konsentrasi Mekatronika Universitas Katolik Parahyangan + - 𝑣𝑠 𝑅 𝑠 𝑅𝑓 + βˆ’ 𝑣 π‘œπ‘£ 𝑝 𝑣 𝑛 Inverting Amplifier Circuit Model 𝑣𝑠 𝑅 𝑠 𝑅𝑓 + βˆ’ 𝑣 π‘œ 𝑣 𝑝 𝑣 𝑛 Tentukan close loop voltage gain 𝐴 = π‘‰π‘œ 𝑉𝑠 ! 𝐴 𝑣 𝑖𝑛 + βˆ’ 𝑣𝑖𝑛 𝑅𝑖𝑛 𝑅 π‘œπ‘’π‘‘
  • 9. Program Studi Teknik Elektro Konsentrasi Mekatronika Universitas Katolik Parahyangan + - Terminal non-inversi dihubungkan ke ground, sehingga 𝑣 𝑝 = 0 maka 𝑣 𝑝 = 𝑣 𝑛 = 0 dan 𝑣𝑠 𝑅 𝑠 𝑅𝑓 + βˆ’ 𝑣 π‘œ 𝑣 𝑝 𝑣 𝑛 𝑣𝑠 βˆ’ 𝑣 𝑛 𝑅 𝑠 βˆ’ 𝑣 𝑛 βˆ’ 𝑣 π‘œ 𝑅𝑓 βˆ’ 𝑖 𝑛 = 0 𝑣𝑠 βˆ’ 𝑣 𝑛 𝑅 𝑠 = 𝑣 𝑛 βˆ’ 𝑣 π‘œ 𝑅𝑓 𝑣𝑠 𝑅𝑓 βˆ’ 𝑣 𝑛 𝑅𝑓 = 𝑣 𝑛 𝑅 𝑠 βˆ’ 𝑣 π‘œ 𝑅 𝑠 𝑣𝑠 𝑅𝑓 = 𝑣 𝑛(𝑅 𝑠 + 𝑅𝑓) βˆ’ 𝑣 π‘œ 𝑅 𝑠 karena 𝑣 𝑛 = 0 𝑣𝑠 𝑅𝑓 = βˆ’ 𝑣 π‘œ 𝑅 𝑠 𝑣 π‘œ 𝑣𝑠 = βˆ’ 𝑅𝑓 𝑅 𝑠 𝐴 = 𝑣 π‘œ 𝑣𝑠 = βˆ’ 𝑅𝑓 𝑅 𝑠 Tentukan close loop voltage gain 𝐴 = 𝑣 π‘œ 𝑣 𝑠 ! Inverting Amplifier KCL di node 𝑣 𝑛: 𝑖1 βˆ’ 𝑖2 βˆ’ 𝑖 𝑛 = 0 𝑖 𝑝 = 𝑖 𝑛 = 0 𝑖 𝑝 𝑖 𝑛 𝐴 𝑣 𝑖𝑛 + βˆ’ 𝑖1 + βˆ’ 𝑖2
  • 10. Program Studi Teknik Elektro Konsentrasi Mekatronika Universitas Katolik Parahyangan 𝑣𝑠 = 0.5 10Ω + βˆ’ 𝑣 π‘œπ‘£ 𝑝 𝑣 𝑛 Contoh Inverting Amplifier 25Ω 1. Tentukan 𝑣 π‘œ 2. Tentukan arus i 𝑣 π‘œ = βˆ’ 𝑅𝑓 𝑅 𝑠 𝑣𝑠 𝑣 π‘œ = βˆ’ 25 10 0.5 𝑣 π‘œ = βˆ’1.25 + βˆ’ 𝑖 𝑖 = 𝑣𝑖 βˆ’ 𝑣 𝑛 𝑅 𝑠 𝑖 = 0.5 βˆ’ 0 10 𝑖 = 0.05 𝐴
  • 11. Program Studi Teknik Elektro Konsentrasi Mekatronika Universitas Katolik Parahyangan 𝑣𝑠 𝑅 𝑠 𝑅𝑓 + βˆ’ 𝑣 π‘œ 𝑣 𝑝 𝑣 𝑛 Tentukan close loop voltage gain 𝐴 = 𝑣 π‘œ 𝑣 𝑠 ! 0 βˆ’ 𝑣 𝑛 𝑅 𝑠 βˆ’ 𝑣 𝑛 βˆ’ 𝑣 π‘œ 𝑅𝑓 βˆ’ 𝑖 𝑛 = 0 βˆ’ 𝑣 𝑛 𝑅 𝑠 = 𝑣 𝑛 βˆ’ 𝑣 π‘œ 𝑅𝑓 βˆ’π‘£π‘  𝑅𝑓 = 𝑣𝑠 𝑅 𝑠 βˆ’ 𝑣 π‘œ 𝑅 𝑠 𝑣 π‘œ 𝑣𝑠 = 𝑅𝑓 + 𝑅 𝑠 𝑅 𝑠 𝑣𝑠(𝑅𝑓 + 𝑅 𝑠) = 𝑣 π‘œ 𝑅 𝑠 Non-Inverting Amplifier Terminal non-inversi dihubungkan ke sumber, sehingga 𝑣 𝑝 = 𝑣𝑠 maka 𝑣 𝑝 = 𝑣 𝑛 = 𝑣𝑠 Op-amp ideal 𝑖 𝑝 = 𝑖 𝑛 = 0 βˆ’ 𝑣𝑠 𝑅 𝑠 = 𝑣𝑠 βˆ’ 𝑣 π‘œ 𝑅𝑓 dan 𝑣 𝑝 = 𝑣 𝑛 = 𝑣𝑠 𝑖 𝑛 𝑖1 𝑖2
  • 12. Program Studi Teknik Elektro Konsentrasi Mekatronika Universitas Katolik Parahyangan Tentukan close loop voltage gain 𝐴 = 𝑣 π‘œ 𝑣 𝑠 ! 0 βˆ’ 𝑣 𝑛 𝑅 𝑠 βˆ’ 𝑣 𝑛 βˆ’ 𝑣 π‘œ 𝑅𝑓 βˆ’ 𝑖 𝑛 = 0 βˆ’ 𝑣 𝑛 𝑅 𝑠 = 𝑣 𝑛 βˆ’ 𝑣 π‘œ 𝑅𝑓 βˆ’π‘£π‘  𝑅𝑓 = 𝑣𝑠 𝑅 𝑠 βˆ’ 𝑣 π‘œ 𝑅 𝑠 𝑣 π‘œ 𝑣𝑠 = 𝑅𝑓 + 𝑅 𝑠 𝑅 𝑠 𝑣𝑠(𝑅𝑓 + 𝑅 𝑠) = 𝑣 π‘œ 𝑅 𝑠 Non-Inverting Amplifier Terminal non-inversi dihubungkan ke sumber, sehingga 𝑣 𝑝 = 𝑣𝑠 maka 𝑣 𝑝 = 𝑣 𝑛 = 𝑣𝑠 Op-amp ideal 𝑖 𝑝 = 𝑖 𝑛 = 0 βˆ’ 𝑣𝑠 𝑅 𝑠 = 𝑣𝑠 βˆ’ 𝑣 π‘œ 𝑅𝑓 dan 𝑣 𝑝 = 𝑣 𝑛 = 𝑣𝑠 𝑅 𝑠 𝑅𝑓 𝑣 𝑝 𝑣 𝑛 + βˆ’ 𝑣 π‘œ
  • 13. Program Studi Teknik Elektro Konsentrasi Mekatronika Universitas Katolik Parahyangan Contoh non-Inverting Amplifier 6𝑉 4Ω 10Ω + βˆ’ 𝑣 π‘œπ‘£ 𝑝 𝑣 𝑛 4𝑉 6 βˆ’ 𝑣 𝑛 𝑅 𝑠 βˆ’ 𝑣 𝑛 βˆ’ 𝑣 π‘œ 𝑅𝑓 βˆ’ 𝑖 𝑛 = 0 Karena 𝑣 𝑝 = 𝑣 𝑛 = 𝑣𝑠 dan 𝑖 𝑝 = 𝑖 𝑛 = 0 6 βˆ’ 4 4 βˆ’ 4 βˆ’ 𝑣 π‘œ 10 βˆ’ 0 = 0 6 βˆ’ 4 4 = 4 βˆ’ 𝑣 π‘œ 10 2 4 = 4 βˆ’ 𝑣 π‘œ 10 5 = 4 βˆ’ 𝑣 π‘œ 𝑣 π‘œ = βˆ’1 1. Tentukan 𝑣 π‘œ KCL di node 𝑣 𝑛
  • 14. Program Studi Teknik Elektro Konsentrasi Mekatronika Universitas Katolik Parahyangan 𝑣𝑠 + βˆ’ 𝑣 π‘œ 𝑣 𝑝 𝑣 𝑛 Buffer Amplifier Terminal non-inversi (𝑣 𝑝) dihubungkan ke sumber, sehingga 𝒗 𝒑= 𝒗 𝒏 maka 𝒗 𝒑 = 𝒗 𝒏 = 𝒗 𝒔 Dan terminal 𝑣 𝑛 terhubung langsung dengan 𝑣𝑠 𝑣 𝑛 = 𝑣𝑠 Sehingga 𝒗 𝒑 = 𝒗 𝒏 = 𝒗 𝒔 = 𝒗 𝒐 Jadi gain loop tertutupnya adalah 1.
  • 15. Program Studi Teknik Elektro Konsentrasi Mekatronika Universitas Katolik Parahyangan Summing Amplifier 𝑣1 𝑅1 𝑅𝑓 + βˆ’ 𝑣 π‘œπ‘£ 𝑝 𝑣 𝑛𝑣2 𝑣3 𝑅2 𝑅3 𝑖1 + 𝑖2 + 𝑖3 βˆ’ 𝑖 = 0 𝑖1 𝑖2 𝑖3 𝑖 𝑣1 βˆ’ 𝑣 𝑛 𝑅1 + 𝑣2 βˆ’ 𝑣 𝑛 𝑅2 + 𝑣3 βˆ’ 𝑣 𝑛 𝑅3 = 𝑣 𝑛 βˆ’ 𝑣 π‘œ 𝑅𝑓 𝑣1 𝑅1 + 𝑣2 𝑅2 + 𝑣3 𝑅3 = βˆ’π‘£ π‘œ 𝑅𝑓 βˆ’ 𝑅𝑓 𝑅1 𝑣1 + 𝑅𝑓 𝑅2 𝑣2 + 𝑅𝑓 𝑅3 𝑣3 = 𝑣 π‘œ Terminal non-inversi dihubungkan ke ground, sehingga 𝑣 𝑝 = 0 maka 𝑣 𝑝 = 𝑣 𝑛 = 0 KCL di node 𝑣 𝑛
  • 16. Program Studi Teknik Elektro Konsentrasi Mekatronika Universitas Katolik Parahyangan 2 𝑉 5Ω 10 Ω + βˆ’ 𝑣 π‘œ 𝑣 𝑝 𝑣 𝑛 1 𝑉 2.5Ω 𝑖1 𝑖2 Contoh Summing Amplifier 2 Ω βˆ’ 10 5 2 + 10 2,5 1 = 𝑣 π‘œ βˆ’ 4 + 4 = 𝑣 π‘œ 1. Tentukan 𝑣 π‘œ 2. Tentukan 𝑖 π‘œ βˆ’8 = 𝑣 π‘œ 𝑖 π‘œ = 𝑣 π‘œ βˆ’ 0 10 + 𝑣 π‘œ βˆ’ 0 2 𝑖 π‘œ = βˆ’ 8 10 βˆ’ 8 2 𝑖 π‘œ = βˆ’0.8 βˆ’ 4 𝑖 π‘œ = βˆ’4.8 𝐴 1. Mentukan 𝑣 π‘œ 1. Mentukan 𝑖 π‘œ 𝑖0
  • 17. Program Studi Teknik Elektro Konsentrasi Mekatronika Universitas Katolik Parahyangan Difference Amplifier 𝑉1 𝑅1 𝑅4 + βˆ’ π‘‰π‘œπ‘‰π‘ 𝑉𝑛 𝑉2 𝑅2 𝑅3 𝑖1 𝑖2
  • 18. Program Studi Teknik Elektro Konsentrasi Mekatronika Universitas Katolik Parahyangan π‘‰π‘œ = 𝑅2 + 𝑅1 𝑅1 𝑉𝑛 βˆ’ 𝑅2 𝑅1 𝑉1 karena 𝑉𝑝 = 𝑉𝑛 π‘‰π‘œ = 𝑅2 + 𝑅1 𝑅1 𝑅4 𝑅3 + 𝑅4 𝑉2 βˆ’ 𝑅2 𝑅1 𝑉1 𝑉𝑝 = 𝑅4 𝑅3 + 𝑅4 𝑉2 𝑉2 βˆ’ 𝑉𝑝 𝑅3 = 𝑉𝑝 𝑅4 𝑉2 𝑅4 βˆ’ 𝑉𝑝 𝑅4 = 𝑉𝑝 𝑅3 𝑉2 𝑅4 = 𝑉𝑝 𝑅3 + 𝑉𝑝 𝑅4 𝑉2 𝑅4 = 𝑉𝑝(𝑅3 + 𝑅4) 𝑉𝑝 = 𝑅4 𝑅3 + 𝑅4 𝑉2 KCL di node 𝑣 𝑝 𝑉1 βˆ’ 𝑉𝑛 𝑅1 = 𝑉𝑛 βˆ’ π‘‰π‘œ 𝑅2 𝑉1 𝑅2 βˆ’ 𝑉𝑛 𝑅2 = 𝑉𝑛 𝑅1 βˆ’ π‘‰π‘œ 𝑅1 π‘‰π‘œ 𝑅1 = 𝑉𝑛 𝑅2 + 𝑅1 βˆ’ 𝑉1 𝑅2 π‘‰π‘œ = 𝑅2 + 𝑅1 𝑅1 𝑉𝑛 βˆ’ 𝑅2 𝑅1 𝑉1 KCL di node 𝑣 𝑛
  • 19. Program Studi Teknik Elektro Konsentrasi Mekatronika Universitas Katolik Parahyangan Cascaded Op Amp Circuits 𝑉𝑠 𝑅 𝑠 𝑅𝑓 + βˆ’ π‘‰π‘œ 𝑉𝑝 𝑉𝑛 𝑉𝑝 𝑉𝑛 𝑅 𝑠 𝑅𝑓 𝑉𝑠 𝑅 𝑠 𝑅𝑓 + βˆ’ π‘‰π‘œ 𝑉𝑝 𝑉𝑛 𝑉𝑝 𝑉𝑛 𝑅 𝑠 𝑅𝑓 Inverting Amplifier Non-Inverting Amplifier
  • 20. Program Studi Teknik Elektro Konsentrasi Mekatronika Universitas Katolik Parahyangan 20mV 3 12 + βˆ’ π‘‰π‘œ 𝑉𝑝 𝑉𝑛 𝑉𝑝 𝑉𝑛 4 10 Op-amp pertama Op-amp kedua 𝑣 π‘œ = 12 + 3 3 20 𝑣 π‘œ = 100π‘šπ‘‰ 𝑣 π‘œ = 10 + 4 4 100 𝑣 π‘œ = 350π‘šπ‘‰