Exercise set

Biomedical Signal Acquisition and Instrumentation Exercises

Worked biomedical engineering exercises for signal acquisition and instrumentation covering SNR, amplifier gain, ADC resolution, sampling, Wheatstone bridges, filtering, uncertainty budgets, leakage current, latency, photodiode front ends, and data integrity.

These exercises practise biomedical signal acquisition and instrumentation as a measurement-chain problem. They cover signal-to-noise ratio, analog front-end gain, ADC resolution, sampling, bridge sensors, filters, uncertainty budgets, leakage current, latency, photodiode circuits, and data integrity.

The goal is not only to calculate an electronics value. The goal is to decide whether a biomedical measurement remains meaningful after the transducer, body interface, analog front end, sampling, processing, safety controls, calibration, and clinical workflow all affect the result.

Assume simplified component behavior unless an exercise states otherwise. Real biomedical instrumentation should also check patient safety, isolation, EMC, motion artefacts, cleaning, sensor placement, software version, calibration state, temperature, humidity, accessory compatibility, data provenance, and validation against intended-use conditions.

How to Use These Exercises

For each instrumentation calculation, define:

  1. the measurand and physiological or biological source;
  2. the transducer and body interface;
  3. the analog front-end, sampling, and processing assumptions;
  4. the safety, uncertainty, and data-integrity limits;
  5. the validation evidence needed before the measurement can support a claim.

The common mistake is treating the sensor datasheet as the device evidence. Biomedical measurement quality is a system property.

Use each result as a measurement-chain screen. A gain, SNR, filter, sampling, leakage, or latency calculation supports engineering review only when the body interface, calibration state, data handling, and acceptance criterion are defined.

Exercise 1: Signal-to-Noise Ratio from Voltage Measurements

A biosignal amplifier measures a desired signal with RMS amplitude:

V_s=2.4\ \text{mV}

The measured RMS noise in the same bandwidth is:

V_n=0.08\ \text{mV}

Assuming equal impedance, calculate SNR as a voltage ratio and in decibels.

Solution

Voltage ratio:

\displaystyle SNR=\frac{V_s}{V_n}=\frac{2.4}{0.08}=30

SNR in decibels:

SNR_{dB}=20\log_{10}(30)=29.5\ \text{dB}

Engineering Comment

The SNR is 30, or 29.5 dB, in the stated bandwidth. That qualifier matters. If bandwidth changes, motion artefacts enter, electrode impedance rises, or cable pickup increases, the SNR can change without any physiological change.

A biomedical SNR value should always state measurement location, bandwidth, sensor setup, and operating condition.

Exercise 2: Analog Front-End Gain and ADC Headroom

A transducer produces a maximum expected differential signal of:

V_{in,max}=1.8\ \text{mV}

The ADC input should use no more than:

V_{ADC,max}=1.2\ \text{V}

to leave headroom for offsets and motion artefacts. Calculate the maximum allowable gain.

Solution

Maximum gain:

\displaystyle G_{max}=\frac{V_{ADC,max}}{V_{in,max}}=\frac{1.2}{0.0018}=666.7

The gain should be no greater than approximately:

G=667

if the 1.8 mV signal is expected at the input.

Engineering Comment

This gain may still be too high if electrode offsets, bridge imbalance, temperature drift, or motion transients appear before filtering. Gain placement should account for saturation risk, not only nominal signal size.

The design should verify the worst credible input, not only the physiological waveform of interest.

Exercise 3: ADC Quantization Step and Input-Equivalent Resolution

A 12-bit ADC has a full-scale input range:

V_{FS}=3.3\ \text{V}

The analog front-end gain is:

G=500

Calculate the ADC voltage step size and the input-equivalent step before amplification.

Solution

Number of ADC codes:

2^{12}=4096

ADC step size:

\displaystyle \Delta_{ADC}=\frac{3.3}{4096}=0.0008057\ \text{V}=0.806\ \text{mV}

Input-equivalent step:

\displaystyle \Delta_{in}=\frac{0.806\ \text{mV}}{500}=0.00161\ \text{mV}=1.61\ \text{microV}

Engineering Comment

The input-equivalent quantization step is about 1.61 microV. That may be adequate for some bioelectric measurements but not all. Effective resolution can be worse because noise, offset, nonlinearity, reference drift, layout, and digital filtering reduce usable precision.

Resolution is not only bits. It is bits used under real signal, noise, and range conditions.

Exercise 4: Sampling Rate Margin

A physiological waveform has clinically relevant content up to:

f_{max}=95\ \text{Hz}

The acquisition system samples at:

f_s=250\ \text{Hz}

Use the sampling condition:

f_s>2f_{max}

Calculate the minimum theoretical sampling rate and the margin.

Solution

Minimum theoretical rate:

2f_{max}=2\times95=190\ \text{Hz}

Margin:

M=f_s-2f_{max}=250-190=60\ \text{Hz}

Engineering Comment

The sampling rate passes the simple criterion with 60 Hz of margin. The review should still check anti-alias filter roll-off, timing jitter, feature timing, dropped samples, and whether abnormal waveforms contain higher frequency content.

Sampling adequacy is a system decision, not only a Nyquist inequality.

Exercise 5: Wheatstone Bridge Output for a Strain Gauge

A quarter-bridge strain gauge has gauge factor:

GF=2.0

The applied strain is:

\epsilon=500\ \text{microstrain}=500\times10^{-6}

Bridge excitation is:

V_{ex}=5.0\ \text{V}

For a small-strain quarter bridge, approximate output is:

\displaystyle V_o\approx\frac{V_{ex}GF\epsilon}{4}

Calculate bridge output.

Solution

Substitute:

\displaystyle V_o\approx\frac{5.0\times2.0\times500\times10^{-6}}{4}
V_o\approx0.00125\ \text{V}=1.25\ \text{mV}

Engineering Comment

The bridge output is only 1.25 mV, so amplifier noise, offset, thermal drift, lead resistance, excitation stability, and mechanical mounting can strongly affect the final measurement.

In biomedical force or pressure measurements, the mechanical interface can dominate as much as the electrical bridge.

Exercise 6: RC Low-Pass Filter Cutoff

A first-order low-pass filter uses:

R=10\ \text{kOhm}

and:

C=0.10\ \text{microF}

Estimate cutoff frequency:

\displaystyle f_c=\frac{1}{2\pi RC}

Solution

Convert values:

R=10{,}000\ \Omega
C=0.10\ \text{microF}=1.0\times10^{-7}\ \text{F}

Cutoff:

\displaystyle f_c=\frac{1}{2\pi(10{,}000)(1.0\times10^{-7})}=159.2\ \text{Hz}

Engineering Comment

The cutoff is about 159 Hz. Whether that is appropriate depends on the signal features and the anti-alias strategy. A filter that is acceptable for trend monitoring may distort timing or morphology for diagnostic interpretation.

Filtering should be validated against the measurement task, not only against a noise target.

Exercise 7: Temperature Measurement Uncertainty Budget

A biomedical temperature channel has the following standard uncertainty components:

ComponentStandard uncertainty
Thermistor calibration0.06 degC
ADC and reference0.03 degC
Sensor self-heating0.04 degC
Contact placement0.08 degC
Ambient sensitivity0.05 degC

Estimate combined standard uncertainty using root-sum-square.

Solution

Combined standard uncertainty:

u_c=\sqrt{0.06^2+0.03^2+0.04^2+0.08^2+0.05^2}
u_c=\sqrt{0.0036+0.0009+0.0016+0.0064+0.0025}
u_c=\sqrt{0.0150}=0.122\ \text{degC}

Engineering Comment

The combined standard uncertainty is about 0.122 degC. The largest contribution is contact placement, not the electronics. That is common in biomedical measurements: the body interface can dominate the error budget.

Improving ADC resolution would not solve the main uncertainty source unless placement and contact are also controlled or monitored.

Exercise 8: Leakage Current from Isolation Resistance

A patient-connected prototype has isolation resistance:

R=150\ \text{MOhm}

under an applied test voltage:

V=250\ \text{V}

Estimate leakage current:

\displaystyle I=\frac{V}{R}

Compare with a project screening limit of 2 microA.

Solution

Convert resistance:

R=150\ \text{MOhm}=150{,}000{,}000\ \Omega

Leakage current:

\displaystyle I=\frac{250}{150{,}000{,}000}=1.667\times10^{-6}\ \text{A}

In microamps:

I=1.667\ \text{microA}

Comparison:

1.667<2

Engineering Comment

The screening calculation passes the project limit, but patient safety review must consider full device configuration, applied parts, humidity, cable routing, accessories, single-fault conditions, insulation materials, and production test methods.

Isolation evidence should be tied to the device configuration being validated.

Exercise 9: Multimodal Latency Alignment

A system records pressure, ECG, and motion data. Estimated processing latencies are:

ChannelLatency
ECG24 ms
Pressure46 ms
Motion31 ms

The analysis algorithm requires channel alignment within:

T_{align}=15\ \text{ms}

Find the maximum latency spread before compensation.

Solution

Maximum latency:

T_{max}=46\ \text{ms}

Minimum latency:

T_{min}=24\ \text{ms}

Latency spread:

T_{spread}=46-24=22\ \text{ms}

Comparison:

22>15

Engineering Comment

The channels are not aligned closely enough before compensation. Timestamp correction, delay calibration, buffering, or algorithm redesign is needed.

Multimodal biomedical analysis can fail when each channel is individually valid but time alignment is weak. The data record should preserve timestamps, sample rates, filter delays, and software version.

Exercise 10: Photodiode Transimpedance Output

A photodiode produces signal current:

I_p=8\ \text{microA}

The transimpedance amplifier feedback resistance is:

R_f=150\ \text{kOhm}

Estimate output magnitude:

V_o=I_pR_f

Then estimate the output if ambient light adds:

I_a=3\ \text{microA}

Solution

Signal-only output:

V_o=8\times10^{-6}\times150{,}000=1.20\ \text{V}

With ambient current:

I_{total}=8+3=11\ \text{microA}
V_{o,total}=11\times10^{-6}\times150{,}000=1.65\ \text{V}

Engineering Comment

The ambient-light contribution raises output from 1.20 V to 1.65 V. If the amplifier or ADC range is narrow, ambient light can consume headroom or create saturation during motion or poor sensor placement.

Optical biomedical sensors should control ambient light, contact pressure, tissue variability, LED drive, photodiode range, and signal-quality indicators.

Exercise 11: Dropped-Sample Rate and Data Integrity

A wearable acquisition system records:

N=720{,}000\ \text{samples}

during a test. The log reports:

N_d=216\ \text{dropped samples}

Calculate the dropped-sample rate in percent. If the project limit is 0.02 percent, does the test pass?

Solution

Dropped-sample rate:

\displaystyle D=\frac{216}{720{,}000}\times100=0.030\%

Comparison:

0.030\%>0.020\%

The test fails the project limit.

Engineering Comment

The failure may look small, but dropped samples can corrupt timing, rhythm analysis, event detection, alarm logic, or multimodal alignment. The team should investigate buffer size, wireless retransmission, storage latency, processor load, power-saving states, timestamp gaps, and how missing data is represented to downstream software.

Data integrity is part of measurement validity.

Review Checklist

When reviewing a biomedical acquisition design, ask:

  • Does the measurement chain include the body interface, not only the sensor?
  • Are gain and filtering chosen for worst-case offsets, artefacts, and saturation?
  • Is SNR stated with bandwidth, location, and operating condition?
  • Does the sampling rate include anti-alias margin, timing, jitter, and feature requirements?
  • Is ADC resolution meaningful after noise, reference error, and effective input range?
  • Does the uncertainty budget include placement, drift, environment, and reference method?
  • Are leakage and isolation checks tied to real device configuration and accessories?
  • Are timestamps, quality flags, calibration state, and software version preserved with data?
  • Are acceptance limits defined before verification data are collected?
  • Can each reported measurement be traced to raw data, preprocessing, calibration, and device configuration?

Biomedical instrumentation is reliable only when the measured number remains traceable, safe, and meaningful in the intended use context.

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See also