Math Bridge: MEMS Acceleration to Capacitance

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Math BridgeSensor ApplicationsStruggle-friendly runway

How does a phone turn gravity into an API number?

One thread from force to spring displacement, differential capacitance, and the reported 9.8 m/s².

Phoebe, the physics guidePhoebe guides
The one targetTrace acceleration through the sensor chain.
The chapter case9.8 m/s², 0.980 nm, 0.0868 fF.
What it buys youRead an API value as measured physics.

A field team has a real problem to settle: How does a phone turn gravity into an API number? They must decide what happens before they change acceleration in metres per second squared on the device. Predict the direction first.

See the relationship first

The figure reads from left to right. The blue card is acceleration in metres per second squared. The middle card uses this page's rule. The green card is proof-mass shift. Follow the arrows: set the input, use the rule, then read the result and its unit.

The audit later on checks more than one number. Here, the added model uses the baseline named below and holds every other chapter value fixed. That sentence bridges the fixtures, so the numbers do not change without a reason.

Acceleration in metres per second squared changes proof-mass shift An input card leads through the page rule to the proof-mass shift result. SET INPUT ONE CONTROL USE RULE predict calculate check units READ RESULT
Follow the arrows. Every stage is linear in this small-displacement model, so doubling acceleration doubles force, displacement, and differential capacitance before calibration recovers a.

Derive the baseline in four moves

  1. 1

    Name the input. The chapter baseline for acceleration in metres per second squared is 9.8.

  2. 2

    Name the rule. F=ma; x=F/k; C0=ε0A/d0; ΔC≈2C0x/d0; a=kx/m

  3. 3

    Put in the chapter value. Set acceleration in metres per second squared to 9.8. The page rule gives proof-mass shift as 0.980 nm.

  4. 4

    Read the result. Keep nm next to the value. Use it only within the limits on this page.

Predict, then change acceleration in metres per second squared

Try Predict what happens to proof-mass shift. Move one control, calculate, then check your idea.

9.8
Chapter baseline
Proof-mass shift

Observe Every stage is linear in this small-displacement model, so doubling acceleration doubles force, displacement, and differential capacitance before calibration recovers a. Reset to 9.8 and compare proof-mass shift.

Explain Only acceleration in metres per second squared moves here. The other chapter values stay fixed.

Check yourself

What should you do before you trust the result?
Answer: Predict its direction, use the shown rule, keep the units, and reset to the worked baseline.
What does this small model leave out?
Answer: Only acceleration in metres per second squared moves. Field effects named in the page limits stay fixed.

1. The API does not touch acceleration

A microscopic proof mass lags behind the phone frame. The chip first senses its displacement, then works backward through a calibrated mechanical and electrical model.

Phoebe: A number can look direct even when several physical conversions sit underneath it.

2. Balance inertia and the spring

1

Write inertial forceF = ma.

2

Write spring forceF = kx after the simple static model settles.

3

Set them equal and divide by kma = kx ⇒ x = ma/k.

Now inspect the proof-mass model before treating x as a number: the spring, damper, mass, and phone frame must have separate roles for the force balance to mean anything physical.

Accelerometer modeled as a spring-mass-damper system: proof mass m suspended from the reference frame by spring k and damper b, displaced by z under acceleration.
Proof-mass mechanics: acceleration moves the reference frame relative to mass m, while spring k and damper b govern displacement z.

Read the diagram from the reference frame into spring k and damper b, then locate proof mass m and displacement z. Frame acceleration creates relative motion; the spring supplies the restoring force kx, and damping limits oscillation. That makes displacement x the mechanical intermediate that the electrical sensing stage can observe.

3. Turn motion into capacitance

C0=ε0A/d0; for small x, ΔCdifferential≈2C0x/d0

One gap shrinks while the opposite gap grows. Their difference reinforces the displacement and rejects changes common to both sides.

Follow the capacitor diagram to connect that moving proof mass to a measurable electrical change: the gap in C = ε0A/d is the physical spacing altered by x.

Capacitive sensing of proof-mass displacement: a voltage source drives a parallel-plate capacitor whose gap g and field E change as the moving plate shifts by z.
Capacitive readout: proof-mass displacement z changes gap g and therefore the capacitance measured across the electric field E.

Start at the voltage source and fixed plate, cross electric field E and gap g, and finish at the moving plate displaced by z. One differential gap closes as the other opens, so their capacitance changes reinforce motion while common effects tend to cancel. Calibration then inverts that electrical change to recover x and, through a = kx/m, acceleration.

4. Try the acceleration

F=ma; x=F/k; C0=ε0A/d0; ΔC≈2C0x/d0; a=kx/m

TryMove acceleration while the chapter's illustrative proof mass, spring, plate area, and gap stay fixed.

Inertial force
Proof-mass shift
One nominal plate
Differential change
Change / C0
Recovered acceleration

ObserveAt 9.8 m/s², the force is 0.980 nN, displacement is 0.980 nm, C0 is 88.5 fF, and the differential change is about 0.0868 fF.

ExplainEvery stage is linear in this small-displacement model, so doubling acceleration doubles force, displacement, and differential capacitance before calibration recovers a.

Technical boundaries.

This is a low-frequency, small-displacement, ideal parallel-plate approximation.

comb fingers
Needs separate evidence
damping
Needs separate evidence
resonance
Needs separate evidence
feedback
Needs separate evidence
parasitics
Needs separate evidence
temperature compensation
Needs separate evidence
cross-axis correction
Needs separate evidence
analogue electronics
Needs separate evidence
ADCs
Needs separate evidence
vendor calibration
Needs separate evidence

Use field evidence or a deeper model before release.

5. Reproduce the resting-phone chain

F=1×10⁻¹⁰×9.8=9.80×10⁻¹⁰ N; x=9.80×10⁻¹⁰ m=0.980 nm
C0=88.5 fF; ΔC≈0.0868 fF≈0.098% of C0

6. Interpret gravity honestly

A resting phone reports about 9.8 m/s² because the supported frame and proof mass have the same relative displacement as an equivalent acceleration. One raw reading cannot distinguish gravity from other sustained acceleration without orientation and motion context.

7. Check yourself

Why is x = ma/k?
Answer: Set the inertial force ma equal to the restoring spring force kx, then divide by k.
Why is the electrical change differential?
Answer: Motion closes one gap and opens the other, so subtracting the two capacitances reinforces the motion signal.
Does a 9.8 m/s² raw value prove hard motion?
Answer: No. A resting sensor also measures the support force associated with gravity.
Honesty boundary.

These are the chapter inputs, worked results, and named teaching assumptions.

0.1 µg mass
Current or responsivity value
1 N/m spring
Distance, wavelength, or size
200 × 100 µm plate
Distance, wavelength, or size
2 µm gap
Distance, wavelength, or size
resulting 0.980 nm / 88.5 fF / 0.0868 fF
Distance, wavelength, or size

They are not vendor specifications; Under the Hood keeps the real sensor and API limits.