MEASUREMENT SYSTEMS
AND THEIR PRINCPLES
Ideal current source: A souce that has infinite output resistance and supply infinite current.
Ideal voltage source: A souce that has zero output impedance and supply infinite current.
Ideal ammeter: A meter that has zero input
resistance and has no voltage drop accross it.
Ideal Voltmeter: A meter that has infinite input resistance and draws no current.
Measuring with ideal instruments 2 1 2 1 2 1
//
R
R
R
R
R
R
R
eq+
=
=
s mV
V =
No measurement errorEffect of source and meter impedances s eq out eq m
V
R
Z
R
V
' '−
=
Ω = = R k R 1 2 1 Ω = M1 in Z Ω = 50 out ZV
V
=
9
.
09
measurement error= 9.1%Keithley Model 2400-C General-Purpose SourceMeter (200V and 1A, 20W)
GPIB interface Boards
Front view Rear view
Keithley Model 2010 7-1/2-Digit, Low-Noise, Autoranging DMM
Digital Multimeters
Oscilloscopes
Analog Oscilloscope
s oc
V
R
R
R
V
2 1 2+
=
2 1 2 1R
R
R
R
R
TH+
=
Thevenin’s Therem:
Given a pairs of terminals in
a linear electrical network, the network may be
replaced by an ideal voltage source V
OCin
series with a resistance R
TH.V
OCis equal to the
open circuit voltage accross terminals, and R
THis the equivalent resistance accross the
terminals when independent voltage sources
are replaced by open circuits.
Norton Equivalent:
Linear network is replaced by
an ideal current source I
SCand the Thevenin
Resistance R
THin parallel with this source. I
SCis
found by calculating the current that would flow
through the terminals if they were shorted
Norton
equivalent
circuit
Thevenin
equivalent
circuit
IMPEDANCE MATCHING
s i L L L V R R R V + =
(
)
2 2 2 S i L L L L L V R R R R V P + = = 0 = L L dR dP i LR
R =
IMPEDANCE MATCHING
ELECTRICAL INTERFACE