Measurement and Instrumentation: cram pack

Formula sheets, the key method steps for every topic and 10 practice problems, with full solutions at the back.

New problemsBack to the course

In the print window, choose “Save as PDF” to keep a copy on your device.

1Formulas and methods

Wheatstone bridge & strain gauges

Divider voltages
Va = VsR2/(R1 + R2), Vb = VsR4/(R3 + R4)
Output
Vab = Va − Vb
Balance
R1/R2 = R3/R4
Slide-wire bridge
R/Rx = l/(100 − l)
Thévenin resistance
Rth = R1∥R2 + R3∥R4
Gauge factor
ΔR/R = GF·ε
Bridge output
quarter Vs·GF·ε/4, half Vs·GF·ε/2, full Vs·GF·ε
Small change, one arm
Vab ≈ Vs·ΔR/(4R)
Stress
σ = E·ε

Method

  1. Treat the bridge as two voltage dividers across the same supply.
  2. For balance, set R₁/R₂ = R₃/R₄ and solve for the unknown resistor.
  3. For an unbalanced bridge, find Va and Vb from the dividers and subtract; use the Thévenin equivalent when a meter loads the output.
  4. For strain gauges, convert strain to ΔR/R = GF·ε and use Vs·GF·ε/4, /2 or ×1 for a quarter, half or full bridge.

Data acquisition & sampling

Nyquist criterion
fs > 2·fmax, fN = fs/2
Alias frequency
fa = |f − k·fs|, k = round(f/fs)
Step size
1 LSB = VFSR/2ᴺ
Quantisation error (rounding)
±½ LSB
Truncating ADC code
D = ⌊Vin/LSB⌋
Bits for a resolution r
2ᴺ ≥ span/r
Ideal SQNR, full-scale sine
SQNR = 6.02·N + 1.76 dB
Data rate
channels × fs × N bit/s
Multiplexed ADC
fs = 1/(n·(tc + tset))
UART
Tb = 1/baud; 8N1 = 10 bits per byte; bytes/s = baud/bits per frame
Baud rate divider
baud = fclk/(16·D)

Method

  1. Write down what is given: sampling rate, signal frequencies, number of bits, input range, baud rate.
  2. For sampling questions, compare each frequency with fs/2; a higher frequency appears at fa = |f − k·fs| with the nearest multiple of fs.
  3. For resolution questions, find 1 LSB = VFSR/2ᴺ, or the smallest N with 2ᴺ ≥ span/resolution.
  4. For data rates and UART links, count everything that is sent: channels, samples per second, bits or whole bytes per sample, and the start, parity and stop bits of every frame.

Op-amp circuits

Inverting amplifier
Vout = −(Rf/Rin)·Vin
Non-inverting amplifier
Vout = (1 + Rf/R1)·Vin
Summing amplifier
Vout = −Rf(V1/R1 + V2/R2)
Ideal op-amp
V+ = V−, Iin = 0

Series & parallel resistors

Resistors in series
Req = R1 + R2 + …
Resistors in parallel
1/Req = 1/R1 + 1/R2 + …
Two in parallel
Req = R1R2 / (R1 + R2)
Ohm's law
V = I·R
Power
P = V·I = I²R = V²/R

Method

  1. Start at the end of the network furthest from the terminals.
  2. Combine resistors in series by adding them, and resistors in parallel with 1/R = 1/R₁ + 1/R₂ + …
  3. Redraw the circuit after each step.
  4. Repeat until one resistor is left between the terminals.

Thévenin & Norton

Thévenin voltage
Vth = Vopen circuit
Thévenin resistance
Rth: all sources off, seen from a–b
Norton current
IN = Vth/Rth
Load current
IL = Vth/(Rth + RL)
Maximum power transfer
RL = Rth, Pmax = Vth²/(4Rth)

Method

  1. Remove the load and mark the two terminals a and b.
  2. Find the open-circuit voltage between a and b: this is Vth.
  3. Switch off all independent sources and find the resistance seen from a–b: this is Rth.
  4. Put the load back on the equivalent circuit: Vth in series with Rth.
  5. For the Norton equivalent, convert: IN = Vth/Rth, with RN = Rth in parallel.

2Practice problems

1.Wheatstone bridge & strain gaugesMedium
+−5 V330 Ω330 Ω + ΔR330 Ω330 Ωab+−Vab​ = ?

A bridge has four 330 Ω arms and Vs = 5 V. The sensor R₂ increases by ΔR = 0.825 Ω. Using the small-change approximation, find the output Vab in mV.

Vs = 5 VR = 330 ΩΔR = 0.825 Ω
Vab = mV
2.Wheatstone bridge & strain gaugesHard
+−5 V350 Ω − ΔR350 Ω + ΔR350 Ω + ΔR350 Ω − ΔRab+−Vo​ = ?

A bridge with 350 Ω arms is excited with 5 V and has four active gauges, two in tension and two in compression (full bridge). The gauge factor is 2 and the strain is 500 µε. Find the bridge output Vo in mV.

Vs = 5 VGF = 2ε = 500 µε
Vo = mV
3.Data acquisition & samplingMedium
SD0​D1​D2​D3​D4​D5​D6​D7​Tb​11·Tb​9600 Bd, 8N2

A UART sends bytes at 9600 baud in the format 8N2: 8 data bits, no parity and 2 stop bit(s), plus the start bit. Find the largest number of data bytes per second it can transfer.

baud = 9600 Bd8N2
RB = B/s
4.Data acquisition & samplingHard
T10 mV/°C×20∿01N = 8, 5 V? °C/LSB

A temperature sensor gives 10 mV/°C (0 V at 0 °C). Its signal is amplified 20 times and fed to an 8-bit ADC with a range of 0 to 5 V (1 LSB = VFSR/2ᴺ). Find the temperature change ΔTLSB that corresponds to one LSB.

S = 10 mV/°CG = 20N = 8VFSR = 5 V
ΔTLSB = °C
5.Op-amp circuitsMedium
−+Vout​R2​ = 22 kΩV1​ = −2.4 VR1​ = 47 kΩV2​ = 1.2 VR3​ = 47 kΩR4​ = 22 kΩ

The difference amplifier uses an ideal op-amp with ±15 V supplies, with R3 = R1 and R4 = R2. Find the output voltage Vout.

V1 = −2.4 VV2 = 1.2 VR1 = R3 = 47 kΩR2 = R4 = 22 kΩ
Vout = V
6.Op-amp circuitsHard
−+Vout​Rf​ = 4.7 kΩV1​ = −0.2 VR1​ = 47 kΩV2​ = 1.5 VR2​ = 1 kΩ

The summing amplifier uses an ideal op-amp with ±15 V supplies. Find the output voltage Vout.

V1 = −0.2 VV2 = 1.5 VR1 = 47 kΩR2 = 1 kΩRf = 4.7 kΩ
Vout = V
7.Series & parallel resistorsMedium
R1​ = 6 ΩR3​ = 8 Ω+−V1​12 VR2​3 ΩAR4​2 ΩB

Find the equivalent resistance Req seen by the source V1.

V1 = 12 VR1 = 6 ΩR2 = 3 ΩR3 = 8 ΩR4 = 2 Ω
Req = Ω
8.Series & parallel resistorsHard
R1​ = 12 ΩR3​ = 12 ΩR5​ = 5 Ω+−V1​30 VR2​6 ΩAR4​6 ΩBR6​2 Ω

Find the equivalent resistance Req seen by the source V1.

V1 = 30 VR1 = 12 ΩR2 = 6 ΩR3 = 12 ΩR4 = 6 ΩR5 = 5 ΩR6 = 2 Ω
Req = Ω
9.Thévenin & NortonMedium
R1​ = 3 ΩR3​ = 10 Ω+−V1​30 VR2​8 ΩAab

Find the Norton current IN: the current that flows from a to b if the terminals are shorted.

V1 = 30 VR1 = 3 ΩR2 = 8 ΩR3 = 10 Ω
IN = A
10.Thévenin & NortonHard
R1​ = 3 ΩR3​ = 5 Ω+−V1​18 VR2​20 ΩAIs​6 ABab

Find the Norton current IN: the current that flows from a to b if the terminals are shorted.

V1 = 18 VIs = 6 AR1 = 3 ΩR2 = 20 ΩR3 = 5 Ω
IN = A

3Solutions

1.Wheatstone bridge & strain gauges

Answer: Vab = 3.125 mV

Wheatstone bridge: two voltage dividers share one supply Vs. The left divider R1–R2 gives Va = Vs·R2/(R1 + R2) and the right divider R3–R4 gives Vb = Vs·R4/(R3 + R4); the output is Vab = Va − Vb. The bridge is balanced (Vab = 0, no current in the meter) when R1/R2 = R3/R4, that is R1·R4 = R2·R3. Seen from the output, the bridge is a Thévenin source with Rth = R1∥R2 + R3∥R4.

Relative change

ΔR/R = 0.825/330 = 0.0025

Linearised output

Vab ≈ 5·0.0025/4 = 3.125 mV

Answer

Vab = 3.125 mV

The exact value is 3.121 mV; the approximation is good while ΔR/R is small.

2.Wheatstone bridge & strain gauges

Answer: Vo = 5 mV

Strain gauges: a gauge changes its resistance with strain: ΔR/R = GF·ε, where the gauge factor GF is about 2 for metal foil. In a bridge with all arms equal to R, one active gauge (quarter bridge) gives Vo ≈ Vs·GF·ε/4. Two active gauges with opposite strains in adjacent arms (half bridge) give Vs·GF·ε/2, and four (full bridge) give Vs·GF·ε. Stress follows from Hooke’s law, σ = E·ε. Load cells state their sensitivity in mV/V: the output at full load per volt of excitation.

Relative resistance change

ΔR/R = 2·500·10⁻⁶ = 0.001

Bridge output

Vo = Vs·GF·ε = 5·0.001 = 5 mV

Answer

Vo = 5 mV
3.Data acquisition & sampling

Answer: RB = 872.7 B/s

UART: an asynchronous serial link sends each byte as a frame: one start bit (low), the data bits, an optional parity bit and one or two stop bits (high). The baud rate is the number of bits per second, so one bit lasts Tb = 1/baud and a frame of n bits lasts n/baud. The common 8N1 format has 10 bits per byte. The baud generator divides the clock: baud = fclk/(16·D) with a whole number D, so the real baud rate differs slightly from the target; an error below about 2 % is usually acceptable.

Bits per frame

1 + 8 + 0 + 2 = 11

Byte rate

9600/11 = 872.7 B/s

Answer

RB = 872.7 B/s
4.Data acquisition & sampling

Answer: ΔTLSB = 0.09766 °C

ADC resolution: an N-bit converter divides its full-scale range VFSR into 2ᴺ codes, from 0 to 2ᴺ − 1. One step is 1 LSB = VFSR/2ᴺ: the smallest change the converter can show. A truncating ADC gives the code ⌊Vin/LSB⌋; a rounding ADC is never more than ½ LSB away from the true value, its quantisation error. Every extra bit halves the LSB and adds about 6 dB to the ideal signal-to-quantisation-noise ratio SQNR = 6.02·N + 1.76 dB for a full-scale sine. To reach a resolution r over a span, choose the smallest N with 2ᴺ ≥ span/r.

Step size

1 LSB = 5000/256 = 19.53 mV

Sensitivity at the ADC

10·20 = 200 mV/°C

Temperature resolution

ΔTLSB = 19.53/200 = 0.09766 °C

Answer

ΔTLSB = 0.09766 °C

The ADC reaches full scale at 25 °C.

5.Op-amp circuits

Answer: Vout = 1.685 V

Ideal op-amp rules: with negative feedback, the op-amp drives its output so that its two inputs sit at the same voltage (V₋ = V₊), and no current flows into either input. Writing KCL at the inverting input with these two facts gives the output.

Voltage at the inputs

R₃ and R₄ carry the same current, so they form a voltage divider; feedback makes V₋ = V₊.

V₊ = V2·R4/(R3 + R4) = 1.2·22/(47 + 22) = 0.3826 V
V₋ = V₊

KCL at the inverting input

(−2.4 − 0.3826)/47 = (0.3826 − Vout)/22
Vout = (R2/R1)·(V2 − V1) = (22/47)·(1.2 − (−2.4)) = 1.685 V

Answer

Vout = 1.685 V
6.Op-amp circuits

Answer: Vout = −7.03 V

Ideal op-amp rules: with negative feedback, the op-amp drives its output so that its two inputs sit at the same voltage (V₋ = V₊), and no current flows into either input. Writing KCL at the inverting input with these two facts gives the output.

Input currents

V₋ = 0, so each input resistor has its full input voltage across it.

I1 = V1/R1 = −0.2/47 = −0.004255 mA
I2 = V2/R2 = 1.5/1 = 1.5 mA
If = I1 + I2 = 1.496 mA

Output voltage

Vout = −Rf·If = −4.7·1.496 = −7.03 V

Answer

Vout = −7.03 V
7.Series & parallel resistors

Answer: Req = 8.308 Ω

Series and parallel resistors: in series the same current flows through each resistor and R = R₁ + R₂ + …. In parallel each resistor has the same voltage and 1/R = 1/R₁ + 1/R₂ + …. A ladder network is reduced one pair at a time until a single equivalent resistance remains.

R1​ = 6 ΩR3​ = 8 Ω+−V1​12 VR2​3 ΩAR4​2 ΩB

Combine resistors from the far end

Start at the end farthest from the source and work back towards it. Resistors carrying the same current are in series; resistors across the same two nodes are in parallel.

R3 + R4 = 8 + 2 = 10 Ω
R2 ∥ 10 = 3·10/(3+10) = 2.308 Ω
Req = R1 + 2.308 = 6 + 2.308 = 8.308 Ω

Answer

Req = 8.308 Ω
8.Series & parallel resistors

Answer: Req = 16.3 Ω

Series and parallel resistors: in series the same current flows through each resistor and R = R₁ + R₂ + …. In parallel each resistor has the same voltage and 1/R = 1/R₁ + 1/R₂ + …. A ladder network is reduced one pair at a time until a single equivalent resistance remains.

R1​ = 12 ΩR3​ = 12 ΩR5​ = 5 Ω+−V1​30 VR2​6 ΩAR4​6 ΩBR6​2 Ω

Combine resistors from the far end

Start at the end farthest from the source and work back towards it. Resistors carrying the same current are in series; resistors across the same two nodes are in parallel.

R5 + R6 = 5 + 2 = 7 Ω
R4 ∥ 7 = 3.231 Ω
R3 + 3.231 = 15.23 Ω
R2 ∥ 15.23 = 4.304 Ω
Req = R1 + 4.304 = 12 + 4.304 = 16.3 Ω

Answer

Req = 16.3 Ω
9.Thévenin & Norton

Answer: IN = 1.791 A

Thévenin’s theorem: any linear two-terminal network behaves like a single voltage source Vth in series with a resistance Rth. Norton’s theorem gives the same network as a current source IN = Vth/Rth in parallel with Rth.

R1​ = 3 ΩR3​ = 10 ΩSHORTR2​8 ΩAabRth​

Find Rth with every source switched off

Replace voltage sources with shorts and current sources with opens, then look into the circuit from a–b.

R1 ∥ R2 = 3·8/(3+8) = 2.182 Ω
Rth = (R1 ∥ R2) + R3 = 2.182 + 10 = 12.18 Ω
R1​ = 3 ΩR3​ = 10 Ω+−V1​30 VR2​8 ΩAab+−Vth​

Find Vth, the open-circuit voltage

With a–b open, no current flows through R₃, so there is no drop across it and V_b = V_A. R₁ and R₂ form a voltage divider.

Vth = V1·R2/(R1+R2) = 30·8/(3+8) = 21.82 V
IN​1.791 ARth​12.18 Ωab

Norton equivalent

A Norton source is the same circuit seen as a current source in parallel with R_th. Its current is the short-circuit current at a–b.

IN = Vth/Rth = 21.82/12.18 = 1.791 A
10.Thévenin & Norton

Answer: IN = 8.057 A

Thévenin’s theorem: any linear two-terminal network behaves like a single voltage source Vth in series with a resistance Rth. Norton’s theorem gives the same network as a current source IN = Vth/Rth in parallel with Rth.

R1​ = 3 ΩR3​ = 5 ΩSHORTR2​20 ΩAOPENBabRth​

Find Rth with every source switched off

Replace voltage sources with shorts and current sources with opens, then look into the circuit from a–b.

R1 ∥ R2 = 3·20/(3+20) = 2.609 Ω
Rth = (R1 ∥ R2) + R3 = 2.609 + 5 = 7.609 Ω
R1​ = 3 ΩR3​ = 5 Ω+−V1​18 VR2​20 ΩAIs​6 ABab+−Vth​

Find Vth, the open-circuit voltage

With a–b open, the only path for Iₛ is through R₃ into node A. Find V_A by superposition of V₁ and Iₛ, then add the drop across R₃.

VA = V1·R2/(R1+R2) + Is·(R1∥R2) = 15.65 + 6·2.609 = 31.3 V
Vth = VB = VA + Is·R3 = 31.3 + 6·5 = 61.3 V
IN​8.057 ARth​7.609 Ωab

Norton equivalent

A Norton source is the same circuit seen as a current source in parallel with R_th. Its current is the short-circuit current at a–b.

IN = Vth/Rth = 61.3/7.609 = 8.057 A

ExamProblems · examproblems.com/courses/measurement-and-instrumentation