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
+−3 V200 Ω200 Ω200 Ω200 Ωab+−

A 200 Ω strain gauge is one arm (R₂) of a bridge with four equal 200 Ω arms and an excitation of 3 V. Find the power Pg dissipated in the gauge, in mW. Self-heating limits the excitation.

Vs = 3 VR = 200 Ω
Pg = mW
2.Wheatstone bridge & strain gaugesHard
+−V350 Ω350 Ω + ΔR350 Ω350 Ωab+−

A 350 Ω strain gauge with gauge factor 2.05 is bonded to a steel bar. Under load its resistance rises by 0.287 Ω. Find the strain ε in microstrain (µε).

R = 350 ΩGF = 2.05ΔR = 0.287 Ω
ε = µε
3.Data acquisition & samplingMedium
Vin​N = ?100 kPa2ᴺ − 10≤ 0.1 kPa

A sensor measures pressure over a span of 100 kPa, and its output fills the whole input range of an ADC. The reading must resolve 0.1 kPa. Find the smallest number of bits N the ADC needs.

span = 100 kParesolution = 0.1 kPa
N =
4.Data acquisition & samplingHard
f0fs​/2fs​8 kHz3f₁?

An 8 kHz square wave is sampled at 20 kHz with no anti-aliasing filter. A square wave contains the odd harmonics 3f₁, 5f₁, 7f₁, … At which frequency fa does its harmonic 3f₁ appear in the sampled data? Give it in kHz.

f₁ = 8 kHzfs = 20 kHzharmonic: 3f₁
fa = kHz
5.Op-amp circuitsMedium
−+Vout​Rf​ = 4.7 kΩVin​R1​ = 2 kΩ

The op-amp is ideal and runs from ±15 V supplies; its output saturates at ±12 V. The inverting amplifier is driven by a sine wave. Find the largest input amplitude Vin,max (peak value) for which the output does not clip.

R1 = 2 kΩRf = 4.7 kΩVsat = ±12 V
Vin,max = V
6.Op-amp circuitsHard
−+Vout​Rf​ = 100 kΩV1​ = −0.9 VR1​ = 47 kΩV2​ = −1.2 VR2​ = 22 kΩ

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

V1 = −0.9 VV2 = −1.2 VR1 = 47 kΩR2 = 22 kΩRf = 100 kΩ
Vout = V
7.Series & parallel resistorsMedium
R1​ = 4 ΩR3​ = 10 Ω+−V1​24 VR2​8 ΩAR4​15 ΩB

Find the equivalent resistance Req seen by the source V1.

V1 = 24 VR1 = 4 ΩR2 = 8 ΩR3 = 10 ΩR4 = 15 Ω
Req = Ω
8.Series & parallel resistorsHard
R1​ = 3 ΩR3​ = 15 ΩR5​ = 4 Ω+−V1​5 VR2​2 ΩAR4​25 ΩBR6​15 Ω

Find the equivalent resistance Req seen by the source V1.

V1 = 5 VR1 = 3 ΩR2 = 2 ΩR3 = 15 ΩR4 = 25 ΩR5 = 4 ΩR6 = 15 Ω
Req = Ω
9.Thévenin & NortonMedium
R1​ = 6 ΩR3​ = 2 Ω+−V1​18 VR2​20 ΩAab

Find the Thévenin voltage Vth seen from terminals a–b.

V1 = 18 VR1 = 6 ΩR2 = 20 ΩR3 = 2 Ω
Vth = V
10.Thévenin & NortonHard
R1​ = 8 ΩR3​ = 10 Ω+−V1​5 VR2​5 ΩAIs​4 ABab

Find the Thévenin voltage Vth seen from terminals a–b.

V1 = 5 VIs = 4 AR1 = 8 ΩR2 = 5 ΩR3 = 10 Ω
Vth = V

3Solutions

1.Wheatstone bridge & strain gauges

Answer: Pg = 11.25 mW

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.

Voltage across the gauge

V = 3/2 = 1.5 V

Power

Pg = 1.5²/200 = 11.25 mW

Answer

Pg = 11.25 mW
2.Wheatstone bridge & strain gauges

Answer: ε = 400 µε

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 = 0.287/350 = 0.00082

Strain

ε = 0.00082/2.05 = 0.0004 = 400 µε

Answer

ε = 400 µε
3.Data acquisition & sampling

Answer: N = 10

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.

Steps needed

100/0.1 = 1000

Bits

log₂(1000) = 9.966
29 = 512 < 1000 ≤ 210 = 1024
N = 10

Answer

N = 10
4.Data acquisition & sampling

Answer: fa = 4 kHz

Sampling: an ADC measures the signal fs times per second. By the Nyquist–Shannon theorem a frequency f is captured correctly only while f < fs/2, the Nyquist (folding) frequency, so the sampling rate must exceed twice the highest signal frequency. A higher frequency is not lost: it shows up as an alias at fa = |f − k·fs|, with the whole number k that brings the result between 0 and fs/2. The samples cannot tell the two apart, so an analogue anti-aliasing filter must remove everything above fs/2 before the ADC.

Harmonic frequency

3f₁ = 3·8 kHz = 24 kHz

Nearest multiple of the sampling rate

m = round(1.2) = 1

Alias frequency

fa = |24 − 1·20| = 4 kHz

Answer

fa = 4 kHz

The alias lands inside the signal band, where no digital filter can remove it. Only an analogue filter before the ADC helps.

5.Op-amp circuits

Answer: Vin,max = 5.106 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.

Gain

|Av| = Rf/R1 = 4.7/2 = 2.35

Largest input before clipping

Vin,max = Vsat/|Av| = 12/2.35 = 5.106 V

Answer

Vin,max = 5.106 V
6.Op-amp circuits

Answer: Vout = 7.369 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 = −0.9/47 = −0.01915 mA
I2 = V2/R2 = −1.2/22 = −0.05455 mA
If = I1 + I2 = −0.07369 mA

Output voltage

Vout = −Rf·If = −100·(−0.07369) = 7.369 V

Answer

Vout = 7.369 V
7.Series & parallel resistors

Answer: Req = 10.06 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​ = 4 ΩR3​ = 10 Ω+−V1​24 VR2​8 ΩAR4​15 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 = 10 + 15 = 25 Ω
R2 ∥ 25 = 8·25/(8+25) = 6.061 Ω
Req = R1 + 6.061 = 4 + 6.061 = 10.06 Ω

Answer

Req = 10.06 Ω
8.Series & parallel resistors

Answer: Req = 4.856 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​ = 3 ΩR3​ = 15 ΩR5​ = 4 Ω+−V1​5 VR2​2 ΩAR4​25 ΩBR6​15 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 = 4 + 15 = 19 Ω
R4 ∥ 19 = 10.8 Ω
R3 + 10.8 = 25.8 Ω
R2 ∥ 25.8 = 1.856 Ω
Req = R1 + 1.856 = 3 + 1.856 = 4.856 Ω

Answer

Req = 4.856 Ω
9.Thévenin & Norton

Answer: Vth = 13.85 V

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​ = 6 ΩR3​ = 2 ΩSHORTR2​20 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 = 6·20/(6+20) = 4.615 Ω
Rth = (R1 ∥ R2) + R3 = 4.615 + 2 = 6.615 Ω
R1​ = 6 ΩR3​ = 2 Ω+−V1​18 VR2​20 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) = 18·20/(6+20) = 13.85 V
10.Thévenin & Norton

Answer: Vth = 54.23 V

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​ = 8 ΩR3​ = 10 ΩSHORTR2​5 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 = 8·5/(8+5) = 3.077 Ω
Rth = (R1 ∥ R2) + R3 = 3.077 + 10 = 13.08 Ω
R1​ = 8 ΩR3​ = 10 Ω+−V1​5 VR2​5 ΩAIs​4 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) = 1.923 + 4·3.077 = 14.23 V
Vth = VB = VA + Is·R3 = 14.23 + 4·10 = 54.23 V

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