TSH330

Noise Measurements

14/19

The input noise of the instrumentation must be extracted from the measured noise value. The real output

noise value of the driver is:

Equation 3

The input noise is called the Equivalent Input Noise as it is not directly measured but is evaluated from the

measurement of the output divided by the closed loop gain (eNo/g).

After simplification of the fourth and the fifth term of

Equation 2 we obtain:

Equation 4

Measurement of the Input Voltage Noise

eN

If we assume a short-circuit on the non-inverting input (R3=0), from

Equation 4 we can derive:

Equation 5

In order to easily extract the value of eN, the resistance R2 will be chosen to be as low as possible. In the

other hand, the gain must be large enough:

R3=0, gain: g=100

Measurement of the Negative Input Current Noise

iNn

To measure the negative input current noise iNn, we set R3=0 and use

Equation 5. This time the gain

must be lower in order to decrease the thermal noise contribution:

R3=0, gain: g=10

Measurement of the Positive Input Current Noise

iNp

To extract iNp from

Equation 3, a resistance R3 is connected to the non-inverting input. The value of R3

must be chosen in order to keep its thermal noise contribution as low as possible against the iNp

contribution:

R3=100W, gain: g=10

eNo

Measured

()

2

instrumentation

()

2

–

=

eNo

2

eN

2

g

2

iNn

2

R2

2

iNp

2

+

×

+

×

R3

2

×

g

2

×

g4kTR2

1

R2

R1

--------

+

2

4kTR3

×

+

×

+

=

eNo

eN

2

g

2

iNn

2

R2

2

g4kTR2

×

+

×

+

×

=