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
+−2 VR1​ = 500 ΩR2​ = 20 ΩR3​ = 150 ΩR4​ = 40 ΩabGRg​ = 50 Ω

A galvanometer with a resistance of 50 Ω is connected between a and b of the bridge shown (Vs = 2 V). Find the galvanometer current Ig from a to b, in µA.

Vs = 2 VR1 = 500 ΩR2 = 20 ΩR3 = 150 ΩR4 = 40 ΩRg = 50 Ω
Ig = µA
2.Wheatstone bridge & strain gaugesHard
+−2.5 V120 Ω120 Ω + ΔR120 Ω120 Ωab+−Vo​

A quarter bridge (one active gauge, GF = 2.12) is excited with 2.5 V. The largest strain to be measured is 1000 µε, and it must give 5 V at the input of an analogue-to-digital converter. Find the amplifier gain G.

Vs = 2.5 VGF = 2.12εmax = 1000 µεVFS = 5 V
G =
3.Data acquisition & samplingMedium
Vin​N = 82.5 V2ᴺ − 101 LSB1.844 V?

An 8-bit ADC with an input range of 0 to 2.5 V truncates: its output code is ⌊Vin/LSB⌋ with 1 LSB = VFSR/2ᴺ. Find the decimal output code D for an input of 1.844 V.

N = 8VFSR = 2.5 VVin = 1.844 V
D =
4.Data acquisition & samplingHard
1216⋮16 ch∿01tc​ = 5 µstset​ = 5 µsfs​ = ?

A 16-channel multiplexer feeds one ADC. Each conversion takes 5 µs, and after every channel switch the input needs 5 µs to settle. The channels are scanned in turn without pause. Find the sampling rate fs of each channel, in kHz.

n = 16tc = 5 µstset = 5 µs
fs = kHz
5.Op-amp circuitsMedium
−+Vout​Rf​ = 10 kΩVin​R1​ = 4.7 kΩ

The op-amp is ideal and runs from ±15 V supplies; its output saturates at ±14 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 = 4.7 kΩRf = 10 kΩVsat = ±14 V
Vin,max = V
6.Op-amp circuitsHard
−+Vout​R2​ = 100 kΩV1​ = −0.5 VR1​ = 1 kΩV2​ = −0.7 VR3​ = 47 kΩR4​ = 100 kΩ

The op-amp is ideal and runs from ±15 V supplies. The resistor ratios are not matched. Find the output voltage Vout.

V1 = −0.5 VV2 = −0.7 VR1 = 1 kΩR2 = 100 kΩR3 = 47 kΩR4 = 100 kΩ
Vout = V
7.Series & parallel resistorsMedium
R1​ = 3 ΩR3​ = 12 Ω+−V1​12 VR2​8 ΩAR4​4 ΩB

Find the equivalent resistance Req seen by the source V1.

V1 = 12 VR1 = 3 ΩR2 = 8 ΩR3 = 12 ΩR4 = 4 Ω
Req = Ω
8.Series & parallel resistorsHard
R1​ = 15 ΩIR1​R3​ = 25 ΩR5​ = 4 Ω+−V1​9 VR2​30 ΩAR4​10 ΩBR6​12 Ω

Find the current IR1 delivered by the source, which flows through R1.

V1 = 9 VR1 = 15 ΩR2 = 30 ΩR3 = 25 ΩR4 = 10 ΩR5 = 4 ΩR6 = 12 Ω
IR1 = A
9.Thévenin & NortonMedium
R1​ = 10 ΩR3​ = 4 Ω+−V1​6 VR2​3 ΩAab

Find the Thévenin resistance Rth seen from terminals a–b.

V1 = 6 VR1 = 10 ΩR2 = 3 ΩR3 = 4 Ω
Rth = Ω
10.Thévenin & NortonHard
R1​ = 6 ΩR3​ = 3 Ω+−V1​36 VR2​20 ΩAIs​4 ABab

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

V1 = 36 VIs = 4 AR1 = 6 ΩR2 = 20 ΩR3 = 3 Ω
Vth = V

3Solutions

1.Wheatstone bridge & strain gauges

Answer: Ig = −3414 µA

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.

Thévenin voltage

Vth = 2·(20/520 − 40/190) = −0.3441 V

Thévenin resistance

Rth = R₁∥R₂ + R₃∥R₄ = 50.81 Ω

Galvanometer current

Ig = −0.3441/(50.81 + 50) = −3414 µA

Answer

Ig = −3414 µA
2.Wheatstone bridge & strain gauges

Answer: G = 3774

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.

Bridge output at full scale

Vo = 1.325 mV

Gain

G = 5/0.001325 = 3774

Answer

G = 3774
3.Data acquisition & sampling

Answer: D = 188

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 = 2.5/28 = 9.766 mV

Code

Vin/LSB = 1844/9.766 = 188.8
code = ⌊188.8⌋ = 188

Answer

D = 188

In binary that is 10111100.

4.Data acquisition & sampling

Answer: fs = 6.25 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

5 + 5 = 10 µs

Time per scan

16·10 = 160 µs

Sampling rate per channel

fs = 1/160 µs = 6.25 kHz

Answer

fs = 6.25 kHz
5.Op-amp circuits

Answer: Vin,max = 6.58 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 = 10/4.7 = 2.128

Largest input before clipping

Vin,max = Vsat/|Av| = 14/2.128 = 6.58 V

Answer

Vin,max = 6.58 V
6.Op-amp circuits

Answer: Vout = 1.905 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₊ = V2·R4/(R3 + R4) = −0.7·100/(47 + 100) = −0.4762 V

Superpose the two inputs

With V₂ = 0, V₁ sees an inverting amplifier. With V₁ = 0, V₊ is amplified by the non-inverting gain 1 + R₂/R₁.

Vout = −(100/1)·(−0.5) + (1 + 100/1)·(−0.4762) = 50 + (−48.1) = 1.905 V

Answer

Vout = 1.905 V
7.Series & parallel resistors

Answer: Req = 8.333 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​ = 12 Ω+−V1​12 VR2​8 ΩAR4​4 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 = 12 + 4 = 16 Ω
R2 ∥ 16 = 8·16/(8+16) = 5.333 Ω
Req = R1 + 5.333 = 3 + 5.333 = 8.333 Ω

Answer

Req = 8.333 Ω
8.Series & parallel resistors

Answer: IR1 = 0.2972 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​ = 25 ΩR5​ = 4 Ω+−V1​9 VR2​30 ΩAR4​10 ΩBR6​12 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 + 12 = 16 Ω
R4 ∥ 16 = 6.154 Ω
R3 + 6.154 = 31.15 Ω
R2 ∥ 31.15 = 15.28 Ω
Req = R1 + 15.28 = 15 + 15.28 = 30.28 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 = 9/30.28 = 0.2972 A

Answer

IR1 = 0.2972 A
9.Thévenin & Norton

Answer: Rth = 6.308 Ω

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​ = 10 ΩR3​ = 4 ΩSHORTR2​3 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 = 10·3/(10+3) = 2.308 Ω
Rth = (R1 ∥ R2) + R3 = 2.308 + 4 = 6.308 Ω
10.Thévenin & Norton

Answer: Vth = 58.15 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​ = 3 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 = 6·20/(6+20) = 4.615 Ω
Rth = (R1 ∥ R2) + R3 = 4.615 + 3 = 7.615 Ω
R1​ = 6 ΩR3​ = 3 Ω+−V1​36 VR2​20 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) = 27.69 + 4·4.615 = 46.15 V
Vth = VB = VA + Is·R3 = 46.15 + 4·3 = 58.15 V

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