---
title: "Vacuum, Charging & Conductive Coatings Interactive Lab | Sandbox Physics"
description: "Can you stop charging without hiding the surface? Only if the charge has a path to ground. A conductive coating drains charge only when it is actually connected to ground. Waiting, or pumping the chamber to a lower pressure, will not remove a layer that has already been deposited on the surface, and that layer can hide the detail you wanted to see."
canonical_url: "https://sandboxphysics.com/labs/electron-vacuum/"
language: "en"
page_type: "lab"
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  zh-CN: "https://sandboxphysics.com/zh/labs/electron-vacuum/"
last_modified: "2026-10-25"
---

E07 · Electron microscopy / specimen physics

# Vacuum, Charging & Conductive Coatings

**Can you stop charging without hiding the surface?** Only if the charge has a path to ground. A conductive coating drains charge only when it is actually connected to ground. Waiting, or pumping the chamber to a lower pressure, will not remove a layer that has already been deposited on the surface, and that layer can hide the detail you wanted to see.

Compare a grounded coating with the same coating disconnected from ground. Run one scan starting from an uncharged surface, then blank the beam: the charge drains away, but the distortion in the scan and the deposited layer stay.

> Interactive simulation: open this page in a web browser to change the parameters and run the model.

Model assumptions

This is an RC circuit model, averaged over the beam duty cycle and started from a fresh surface; it is not recorded SEM data. The capacitance is fixed and the net current is negative. The coating's continuity and conductance are assumed. Beam-induced deposition stops during recovery, but material already deposited stays. Gas transmission, scan displacement, surface masking and the spectral markers are illustrative. Ripple from individual pixel pulses, neutralization by gas ions, positive charging, self-consistent fields and material calibration are not modeled.

Physics tutorial

## Can you stop charging without hiding the surface?

**Background** Compare a grounded coating with the same coating disconnected from ground. Run one scan starting from an uncharged surface, then blank the beam: the charge drains away, but the distortion in the scan and the deposited layer stay.

**Why it matters** A conductive coating needs a path to ground. Waiting after an unstable scan does not correct the image already formed.

Start with the essentials

- **Focus question**: Does a coating still drain charge when its ground contact is open?
- **One-sentence intuition**: What matters for the image is the charge during the scan, not what is left after blanking, and neither waiting nor lower pressure removes a layer already deposited.

### Core mathematical model

#### Charging up from an uncharged surface

$$
C\frac{dV}{dt}=-I_{\mathrm{net}}-GV,\qquad V(t)=-\frac{I_{\mathrm{net}}}{G}\left(1-e^{-t/\tau_c}\right),\quad \tau_c=\frac{C}{G}
$$

The capacitance is fixed at 2 pF. The net negative current is 35 percent of the incident current, times the duty fraction. That averaged duty fraction comes from the dwell time and an assumed 10 microsecond blanking interval per pixel; the rapid on-off switching itself is not resolved.

#### Charge draining after the beam is off

$$
V(T+t_{\mathrm{off}})=V(T)e^{-t_{\mathrm{off}}/\tau_c},\qquad G=G_0+cG_{\mathrm{coat}}
$$

The contact switch is one when the coating is connected and zero when it is open. The bare specimen's own leakage stays in both cases. Conductance here means the effective path to ground, not the bulk conductivity. Waiting changes the final potential, not the scan that came before.

#### Deposited layer and surface masking

$$
h(t)=r_{\mathrm{dep}}\min(t,T),\qquad S(t)=\exp\left[-\frac{b_{\mathrm{coat}}+h(t)}{15\,\mathrm{nm}}\right]
$$

Only beam-induced deposition is modeled, and material already deposited stays during recovery. Each scan row uses the state of the surface at the time that row was scanned. The masking and the displacement scale are illustrative; they are not a resolution calibration or an electrostatic transport calculation.

### Common difficulties

#### Waiting afterwards does not fix the image

**Typical misconception** A small final potential means the preceding scan was stable.

**Better mental model** The target uses the potential at the end of the scan. The recovery time does not change the scan image, and it does not clean away deposited material.

#### What the model covers

**Typical misconception** This is a calibrated SEM charging or coating calculation.

**Better mental model** This is an RC circuit model, averaged over the beam duty cycle and started from a fresh surface; it is not recorded SEM data. The capacitance is fixed and the net current is negative. The coating's continuity and conductance are assumed. Beam-induced deposition stops during recovery, but material already deposited stays. Gas transmission, scan displacement, surface masking and the spectral markers are illustrative. Ripple from individual pixel pulses, neutralization by gas ions, positive charging, self-consistent fields and material calibration are not modeled.

### Run the experiment

1. 01

   #### Compare a grounded and a floating coating

   Select Thin carbon coat, then Disconnected coat. The film thickness and masking stay the same, but the charge drainage changes.

   **What to observe:** A floating coating still shows its spectral marker and still masks the surface, but it no longer adds a path to ground.

2. 02

   #### Blank the beam after the scan

   Select Bare scan, then blank. Compare the potential at the end of the scan with the final residual potential, then change the Beam-off recovery duration.

   **What to observe:** The charge decays once the beam is off, but the scan image and the contamination stay the same, and an unstable exposure still fails the target.

3. 03

   #### Find a stable preparation

   During the scan, keep the potential's magnitude below 2 V, the contamination layer below 1 nm and the surface contrast above 75 percent. Recovering afterwards cannot make an unstable exposure pass.

   **What to observe:** A thin, grounded carbon coat meets this teaching target. Thick gold hides surface detail, and a poor vacuum raises the assumed deposition rate. Lowering the pressure alone does not ground an insulator.

Physical conclusion

Make the scan itself stable. Specimen preparation, what happened during the scan and the charge left at the end are three separate things.

Fields & matter · Starter path

## From a field to an electron microscope

Map an electric field and steer a charged particle. Then find the electron's wavelength and use electron beams to see a crystal and a surface.

[Start here → **Make an Electric Field Visible** Move the probe around a dipole and check that the field always points downhill on the potential landscape. Observe · 8 min](https://sandboxphysics.com/labs/electric-field/)

1. [1 Make an Electric Field Visible](https://sandboxphysics.com/labs/electric-field/)
2. [2 A Charge Bending through Fields](https://sandboxphysics.com/labs/charged-particle/)
3. [3 Electron Wavelength & Voltage](https://sandboxphysics.com/labs/electron-wavelength/)
4. [4 Electron Diffraction & Reciprocal Space](https://sandboxphysics.com/labs/electron-diffraction/)
5. [5 TEM Bright Field, Dark Field & SAED](https://sandboxphysics.com/labs/tem-mode-selector/)
6. [6 SEM Secondary-Electron Topography](https://sandboxphysics.com/labs/sem-topography/)

[View the full path →](https://sandboxphysics.com/topics/fields-and-matter/#starter-path)