Measurement and Instrumentation: cram pack

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

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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 V100 Ω100 Ω + ΔR100 Ω100 Ωab+−141.5 mV

A bridge with four 100 Ω arms is supplied with 5 V. When the sensor R₂ changes, the output reads Vab = 141.5 mV. Find the exact change ΔR of R₂.

Vs = 5 VR = 100 ΩVab = 141.5 mV
ΔR = Ω
2.Wheatstone bridge & strain gaugesHard
+−3 V350 Ω350 Ω + ΔR350 Ω350 Ωab+−0.769 mV

A strain gauge (GF = 2.05) on a member with E = 210 GPa forms a quarter bridge excited with 3 V. The output reads 0.769 mV. Find the axial stress σ in MPa.

Vs = 3 VGF = 2.05Vo = 0.769 mVE = 210 GPa
σ = MPa
3.Data acquisition & samplingMedium
Vin​N = ?5 V2ᴺ − 10≤ 5 mV

An ADC with an input range of 0 to 5 V must resolve steps of 5 mV or smaller. Find the smallest number of bits N.

VFSR = 5 Vresolution = 5 mV
N =
4.Data acquisition & samplingHard
1216⋮16 ch∿01tc​ = 10 µstset​ = 2 µsfs​ = ?

A 16-channel multiplexer feeds one ADC. Each conversion takes 10 µs, and after every channel switch the input needs 2 µs to settle. The channels are scanned in turn without pause. Find the sampling rate fs of each channel, in kHz.

n = 16tc = 10 µstset = 2 µs
fs = kHz
5.Op-amp circuitsMedium
−+Vout​Rf​ = 10 kΩR1​ = 10 kΩVin​ = 4 VRa​ = 47 kΩRb​ = 2 kΩ

The op-amp is ideal and runs from ±15 V supplies. Find the output voltage Vout.

Vin = 4 VRa = 47 kΩRb = 2 kΩR1 = 10 kΩRf = 10 kΩ
Vout = V
6.Op-amp circuitsHard
−+Vout​C = 4.7 µFVin​ = 1.2 VR = 1 kΩ

The integrator uses an ideal op-amp with ±15 V supplies; its output saturates at ±14 V. The capacitor is uncharged when a constant input Vin = 1.2 V is applied at t = 0. Find the output voltage Vout at t = 20 ms.

Vin = 1.2 VR = 1 kΩC = 4.7 µFVsat = ±14 Vt = 20 ms
Vout = V
7.Series & parallel resistorsMedium
R1​ = 5 ΩR3​ = 15 Ω+−V1​12 VR2​8 ΩAR4​3 ΩB

Find the equivalent resistance Req seen by the source V1.

V1 = 12 VR1 = 5 ΩR2 = 8 ΩR3 = 15 ΩR4 = 3 Ω
Req = Ω
8.Series & parallel resistorsHard
R1​ = 15 ΩR3​ = 5 ΩR5​ = 20 Ω+−V1​10 VR2​2 ΩIR2​AR4​4 ΩBR6​25 Ω

Find the current IR2 through R2.

V1 = 10 VR1 = 15 ΩR2 = 2 ΩR3 = 5 ΩR4 = 4 ΩR5 = 20 ΩR6 = 25 Ω
IR2 = A
9.Thévenin & NortonMedium
R1​ = 15 ΩR3​ = 12 Ω+−V1​24 VR2​8 ΩAab

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

V1 = 24 VR1 = 15 ΩR2 = 8 ΩR3 = 12 Ω
IN = A
10.Thévenin & NortonHard
R1​ = 8 ΩR3​ = 5 Ω+−V1​5 VR2​3 ΩAIs​2 ABab

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

V1 = 5 VIs = 2 AR1 = 8 ΩR2 = 3 ΩR3 = 5 Ω
IN = A

3Solutions

1.Wheatstone bridge & strain gauges

Answer: ΔR = 12 Ω

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.

Node voltage

Va = 2.5 + 0.1415 = 2.642 V

Solve the divider

R₂ = 100·2.642/(5 − 2.642) = 112 Ω
ΔR = 112 − 100 = 12 Ω

Answer

ΔR = 12 Ω
2.Wheatstone bridge & strain gauges

Answer: σ = 105 MPa

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.

Strain

ε = 4·0.000769/(3·2.05) = 0.0005002

Stress

σ = 210·10³ MPa·0.0005002 = 105 MPa

Answer

σ = 105 MPa
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

5000 mV/5 mV = 1000

Bits

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

Answer

N = 10
4.Data acquisition & sampling

Answer: fs = 5.208 kHz

Data rates: every channel delivers fs samples per second of N bits, so the raw rate is channels × fs × N bit/s. In memory a sample takes whole bytes (a 12-bit sample is stored in 2 bytes), so the memory for a recording is channels × fs × bytes per sample × time. A multiplexed ADC converts the channels one after another: each conversion (with settling) takes t, so one round of n channels takes n·t and each channel is sampled at 1/(n·t).

Time per channel

10 + 2 = 12 µs

Time per scan

16·12 = 192 µs

Sampling rate per channel

fs = 1/192 µs = 5.208 kHz

Answer

fs = 5.208 kHz
5.Op-amp circuits

Answer: Vout = 0.3265 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 + input

V₊ = Vin·Rb/(Ra + Rb) = 4·2/(47 + 2) = 0.1633 V

Non-inverting gain

V₋ = V₊, and the current through R₁ also flows through Rf.

Vout = V₊·(1 + Rf/R1) = 0.1633·(1 + 10/10) = 0.3265 V

Answer

Vout = 0.3265 V
6.Op-amp circuits

Answer: Vout = −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.

Input current and ramp rate

kΩ times µF gives milliseconds.

RC = 1 kΩ · 4.7 µF = 4.7 ms
ramp rate = −Vin/(RC) = −1.2/4.7 = −0.2553 V/ms

Output at the given time

The ideal value lies inside ±Vsat, so the integrator has not clipped yet.

Vout = −Vin·t/(RC) = −1.2·20/4.7 = −5.106 V

Answer

Vout = −5.106 V
7.Series & parallel resistors

Answer: Req = 10.54 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​ = 5 ΩR3​ = 15 Ω+−V1​12 VR2​8 ΩAR4​3 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 = 15 + 3 = 18 Ω
R2 ∥ 18 = 8·18/(8+18) = 5.538 Ω
Req = R1 + 5.538 = 5 + 5.538 = 10.54 Ω

Answer

Req = 10.54 Ω
8.Series & parallel resistors

Answer: IR2 = 0.4888 A

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​ = 15 ΩR3​ = 5 ΩR5​ = 20 Ω+−V1​10 VR2​2 ΩAR4​4 ΩBR6​25 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 = 20 + 25 = 45 Ω
R4 ∥ 45 = 3.673 Ω
R3 + 3.673 = 8.673 Ω
R2 ∥ 8.673 = 1.625 Ω
Req = R1 + 1.625 = 15 + 1.625 = 16.63 Ω

Current from the source

The source sees only Req, so Ohm’s law gives the current it delivers. That current flows through R₁.

IR1 = V1/Req = 10/16.63 = 0.6015 A

Current through R₂

Subtract the drop across R₁ to get the voltage at node A, which is the voltage across R₂.

VA = V1 − IR1·R1 = 10 − 0.6015·15 = 0.9776 V
IR2 = VA/R2 = 0.9776/2 = 0.4888 A

Answer

IR2 = 0.4888 A
9.Thévenin & Norton

Answer: IN = 0.4848 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​ = 15 ΩR3​ = 12 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 = 15·8/(15+8) = 5.217 Ω
Rth = (R1 ∥ R2) + R3 = 5.217 + 12 = 17.22 Ω
R1​ = 15 ΩR3​ = 12 Ω+−V1​24 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) = 24·8/(15+8) = 8.348 V
IN​0.4848 ARth​17.22 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 = 8.348/17.22 = 0.4848 A
10.Thévenin & Norton

Answer: IN = −1.81 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​ = 8 ΩR3​ = 5 ΩSHORTR2​3 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 = 8·3/(8+3) = 2.182 Ω
Rth = (R1 ∥ R2) + R3 = 2.182 + 5 = 7.182 Ω
R1​ = 8 ΩR3​ = 5 Ω+−V1​5 VR2​3 ΩAIs​2 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) = 1.364 + (−2)·2.182 = −3 V
Vth = VB = VA + Is·R3 = −3 + (−2)·5 = −13 V
IN​1.81 ARth​7.182 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 = −13/7.182 = −1.81 A

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