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
+−3 V150 Ω150 Ω + ΔR150 Ω150 Ωab+−Vab​ = ?

A bridge has four 150 Ω arms and Vs = 3 V. The sensor R₂ increases by ΔR = 0.75 Ω. Using the small-change approximation, find the output Vab in mV.

Vs = 3 VR = 150 ΩΔR = 0.75 Ω
Vab = mV
2.Wheatstone bridge & strain gaugesHard
+−3 V1000 Ω1000 Ω + ΔR1000 Ω1000 Ωab+−Vo​ = ?

A bridge with 1000 Ω arms is excited with 3 V and has one active gauge (quarter bridge). The gauge factor is 2.12 and the strain is 600 µε. Find the bridge output Vo in mV.

Vs = 3 VGF = 2.12ε = 600 µε
Vo = mV
3.Data acquisition & samplingMedium
SD0​D1​D2​D3​D4​D5​D6​D7​Tb​10·Tb​19200 Bd, 8N1

A UART sends bytes at 19200 baud in the format 8N1: 8 data bits, no parity and 1 stop bit(s), plus the start bit. Find the largest number of data bytes per second it can transfer.

baud = 19200 Bd8N1
RB = B/s
4.Data acquisition & samplingHard
SD0​D1​D2​D3​D4​D5​D6​D7​Tb​10·Tb​115200 Bd, 8N1

A 12-bit ADC streams every sample over a UART at 115200 baud, format 8N1 (start bit, 8 data bits, 1 stop bit). Each sample is sent as 2 whole byte(s) and the link is busy all the time. Find the highest signal frequency fmax that can be sampled without aliasing, in Hz.

baud = 115200 BdN = 128N1
fmax = Hz
5.Op-amp circuitsMedium
−+Vout​Rf​ = 4.7 kΩR1​ = 1 kΩVin​ = −1.4 V

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

Vin = −1.4 VR1 = 1 kΩRf = 4.7 kΩ
Vout = V
6.Op-amp circuitsHard
Vin​V1​Vout​stage 1: invertingR1​ = 10 kΩRf1​ = 22 kΩstage 2: non-invertingR2​ = 47 kΩRf2​ = 10 kΩ

Two ideal op-amp stages are connected in cascade: an inverting amplifier (R1, Rf1) followed by a non-inverting amplifier (R2 to ground, Rf2 in the feedback). Both run from ±15 V supplies. Find the overall voltage gain Av = Vout/Vin.

R1 = 10 kΩRf1 = 22 kΩR2 = 47 kΩRf2 = 10 kΩ
Av =
7.Series & parallel resistorsMedium
R1​ = 15 ΩR3​ = 2 Ω+−V1​30 VR2​4 ΩAR4​5 ΩB

Find the equivalent resistance Req seen by the source V1.

V1 = 30 VR1 = 15 ΩR2 = 4 ΩR3 = 2 ΩR4 = 5 Ω
Req = Ω
8.Series & parallel resistorsHard
R1​ = 2 ΩIR1​R3​ = 30 ΩR5​ = 2 Ω+−V1​24 VR2​10 ΩAR4​25 ΩBR6​12 Ω

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

V1 = 24 VR1 = 2 ΩR2 = 10 ΩR3 = 30 ΩR4 = 25 ΩR5 = 2 ΩR6 = 12 Ω
IR1 = A
9.Thévenin & NortonMedium
R1​ = 4 ΩR3​ = 10 Ω+−V1​12 VR2​8 ΩARL​20 ΩIL​B

A load RL = 20 Ω is connected across a–b. Replace the rest of the circuit with its Thévenin equivalent and find the load current IL.

V1 = 12 VR1 = 4 ΩR2 = 8 ΩR3 = 10 ΩRL = 20 Ω
IL = A
10.Thévenin & NortonHard
R1​ = 20 ΩR3​ = 6 Ω+−V1​18 VR2​5 ΩAIs​5 ABRL​12 ΩIL​

A load RL = 12 Ω is connected across a–b. Replace the rest of the circuit with its Thévenin equivalent and find the load current IL.

V1 = 18 VIs = 5 AR1 = 20 ΩR2 = 5 ΩR3 = 6 ΩRL = 12 Ω
IL = A

3Solutions

1.Wheatstone bridge & strain gauges

Answer: Vab = 3.75 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 = 0.75/150 = 0.005

Linearised output

Vab ≈ 3·0.005/4 = 3.75 mV

Answer

Vab = 3.75 mV

The exact value is 3.741 mV; the approximation is good while ΔR/R is small.

2.Wheatstone bridge & strain gauges

Answer: Vo = 0.954 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 = 2.12·600·10⁻⁶ = 0.001272

Bridge output

Vo ≈ Vs·GF·ε/4 = 3·0.001272/4 = 0.954 mV

Answer

Vo = 0.954 mV
3.Data acquisition & sampling

Answer: RB = 1920 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 + 1 = 10

Byte rate

19200/10 = 1920 B/s

Answer

RB = 1920 B/s
4.Data acquisition & sampling

Answer: fmax = 2880 Hz

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 sample on the line

2·10 = 20 bit

Highest sampling rate

fs,max = 115200/20 = 5760 Hz

Nyquist limit

fmax = 5760/2 = 2880 Hz

Answer

fmax = 2880 Hz
5.Op-amp circuits

Answer: Vout = −7.98 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.

Inverting input follows the input

V₋ = V₊ = −1.4 V
I = V₋/R1 = −1.4/1 = −1.4 mA

Output voltage

The current through R₁ also flows through Rf.

Vout = V₋ + I·Rf = −1.4 + (−1.4)·4.7 = −7.98 V

Answer

Vout = −7.98 V
6.Op-amp circuits

Answer: Av = −2.668

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 of each stage

A1 = −Rf1/R1 = −22/10 = −2.2
A2 = 1 + Rf2/R2 = 1 + 10/47 = 1.213

Overall gain

Av = A1·A2 = −2.2·1.213 = −2.668

Answer

Av = −2.668
7.Series & parallel resistors

Answer: Req = 17.55 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​ = 15 ΩR3​ = 2 Ω+−V1​30 VR2​4 ΩAR4​5 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 = 2 + 5 = 7 Ω
R2 ∥ 7 = 4·7/(4+7) = 2.545 Ω
Req = R1 + 2.545 = 15 + 2.545 = 17.55 Ω

Answer

Req = 17.55 Ω
8.Series & parallel resistors

Answer: IR1 = 2.41 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​ = 2 ΩR3​ = 30 ΩR5​ = 2 Ω+−V1​24 VR2​10 ΩAR4​25 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 = 2 + 12 = 14 Ω
R4 ∥ 14 = 8.974 Ω
R3 + 8.974 = 38.97 Ω
R2 ∥ 38.97 = 7.958 Ω
Req = R1 + 7.958 = 2 + 7.958 = 9.958 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 = 24/9.958 = 2.41 A

Answer

IR1 = 2.41 A
9.Thévenin & Norton

Answer: IL = 0.2449 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​ = 4 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 = 4·8/(4+8) = 2.667 Ω
Rth = (R1 ∥ R2) + R3 = 2.667 + 10 = 12.67 Ω
R1​ = 4 ΩR3​ = 10 Ω+−V1​12 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) = 12·8/(4+8) = 8 V
Rth​ = 12.67 Ω+−Vth​8 VRL​20 ΩIL​

Connect the load to the Thévenin equivalent

The Thévenin source and R_th in series behave exactly like the original circuit at a–b, so the load sees a simple series loop.

IL = Vth/(Rth + RL) = 8/(12.67 + 20) = 0.2449 A
10.Thévenin & Norton

Answer: IL = −2.109 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​ = 20 ΩR3​ = 6 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 = 20·5/(20+5) = 4 Ω
Rth = (R1 ∥ R2) + R3 = 4 + 6 = 10 Ω
R1​ = 20 ΩR3​ = 6 Ω+−V1​18 VR2​5 ΩAIs​5 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) = 3.6 + (−5)·4 = −16.4 V
Vth = VB = VA + Is·R3 = −16.4 + (−5)·6 = −46.4 V
Rth​ = 10 Ω−+Vth​46.4 VRL​12 ΩIL​

Connect the load to the Thévenin equivalent

The Thévenin source and R_th in series behave exactly like the original circuit at a–b, so the load sees a simple series loop.

IL = Vth/(Rth + RL) = −46.4/(10 + 12) = −2.109 A

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