Solutions for Assignment 3 - Analog Electronics | ECE 3050, Assignments of Electrical and Electronics Engineering

Material Type: Assignment; Class: Analog Electronics; Subject: Electrical & Computer Engr; University: Georgia Institute of Technology-Main Campus; Term: Spring 2004;

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ECE 3050 – Spring 2004 Page 1
Homework Assignment No. 3 - Solution
1.) The differential amplifier below uses an ideal op amp. Find the values of R1, R2, R3
and R4 if the single-ended input resistances, Rin1 and Rin2 are to be 100k and the output
voltage is to be vout = 10(v1v2).
+
-
R
1
R
3
R
4
R
2
v
out
=
10(v
1
-v
2
)
-
+
v
2
v
1
R
in2
R
in1
Fig. S03Q03P1
Solution
The first step is to find vout as a function of v1 and v2 and to find Rin1 and Rin2.
The output voltage can be found by using superposition applied to the inputs v1 and v2.
The result is,
vout =
vout
v1
|
v2=0 +
vout
v2
|
v1=0 =
R1+R2
R1
R4
R3+ R4
v1 -
R2
R1
v2
Rin1 = R3 + R4 (remember to set v2 to zero in this calculation – only one
excitation at a time)
Rin2 = R1 (remember to set v1 to zero in this calculation – only one excitation at a
time)
From the input resistance results, we can write that,
R3 + R4 = 100k and R1 = 100k
Substituting these values in the voltage gain expression gives,
vout =
R1+R2
100k
R4
100k v1 -
R2
100k v2 = 10(v1v2)
This gives us R2 = 1M. Substituting this back into the voltage gain expression gives,
vout =
1100k
100k
R4
100k v1 - 10 v2 = 10(v1v2) R4 = 1000k
11 = 90.9k
Since the sum of R3 and R4 must equal 100k, we get
R3 = 100k - 90.9k = 9.1k
Substituting these values back into the top three equations satisfies the requirements.
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Homework Assignment No. 3 - Solution

1.) The differential amplifier below uses an ideal op amp. Find the values of R 1 , R 2 , R 3 and R 4 if the single-ended input resistances, R (^) in 1 and R (^) in 2 are to be 100kΩ and the output voltage is to be vout = 10( v 1 – v 2 ).

R 1 -

R 3

R 4

R 2

v (^) out =

  • 10( v 1 - v 2 )

v 2 v 1

R (^) in 2

R (^) in 1

Fig. S03Q03P

Solution

The first step is to find v (^) out as a function of v 1 and v 2 and to find R (^) in 1 and R (^) in 2.

The output voltage can be found by using superposition applied to the inputs v 1 and v 2. The result is,

v (^) out = 

v (^) outv 1

v 2 =0 +^ 

v (^) outv 2

v 1 =0 =^ 

R 1 + R 2 

R 1 

R 4 

R 3 + R 4 v^1 -^ 

R 2 

R 1 v^2

R (^) in 1 = R 3 + R 4 (remember to set v 2 to zero in this calculation – only one excitation at a time) R (^) in 2 = R 1 (remember to set v 1 to zero in this calculation – only one excitation at a time)

From the input resistance results, we can write that,

R 3 + R 4 = 100kΩ and R 1 = 100kΩ

Substituting these values in the voltage gain expression gives,

v (^) out = (^) 

R 1 + R 2 

100kΩ (^) 

R 4 

100kΩ v^1 -^ 

R 2 

100kΩ v^2 = 10( v^1 –^ v^2 )

This gives us R 2 = 1MΩ. Substituting this back into the voltage gain expression gives,

v (^) out = (^) 

1100kΩ 100kΩ 

R 4 

100kΩ v^1 - 10^ v^2 = 10( v^1 –^ v^2 )^ →^ R^4 =

1000kΩ 11 = 90.9kΩ

Since the sum of R 3 and R 4 must equal 100kΩ, we get

R 3 = 100kΩ - 90.9kΩ = 9.1kΩ

Substituting these values back into the top three equations satisfies the requirements.

2.) Assume that the op amps are ideal and find i (^) out as a function of the inputs, v 1 and v 2. Find the input resistance defined as Rin = ( v 2 - v 1 )/ i (^) in.

ZL

iin iout

iin

v 2

v 1

R 1

R 1

R 2

R 2

R 3

A

A

Rin

F02Q03S

i 2 i 3

i 2

Solution

From the circuit we can write the following equations based on an ideal op amp:

i (^) out = i 3 , v 2 – v 1 = 2 R 1 i (^) in , i 2 R 2 + i 2 R 2 = i 3 R 3, i (^) in = - i 2

i (^) out = i 3 =

2 R 2 i 2 R 3 =

2 R 2

R 3 (-^ i^ in ) =

2 R 2

R 3 

v 2 – v 1 2 R 1 =^

R 2

R 1 R 3 (^ v^1 –^ v^2 )

i (^) out =

R 2

R 1 R 3 (^ v^1 –^ v^2 )

The input resistance, R (^) in is seen to be equal to 2 R 1. R (^) in = 2 R 1

3.) Problem 11.38 (12.24) of the text

Applying op-amp assumption 1 to the circuit on the next page, the voltage at the top of R 2 is v (^) O2 , and applying op-amp assumption 2,

vS R (^1) = − vO R (^2) or v (^) O2 = −v (^) S^ R^2 R (^1) Since the op-amp input currents are zero, and i = v R^ S 1

, v (^) O1 = −iR 2 − iR 3 = − RR^2 1

  • RR^3 1

 ^

 ^ v (^) S

Alternatively, the voltage at the bottom of R2 is zero, so

v (^) O1 = 1 + RR^3 2

 ^

 ^ v (^) O2 = 1 + RR^3 2

 ^

 ^ − RR^2 1

 ^

 ^ v (^) S = − RR^2 1

  • RR^3 1

 ^

 ^ v (^) S

See next page for figure