Experiment Schematics: Difference between revisions

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[[File:hall_good_example.png]]
[[File:hall_good_example.png]]


Here we have a simple metallic strip with clearly labelled current (<math>I</math>) as well as magnetic field (<math>B</math>) and hall voltage (<math>V_H</math>). Then you can relate this to the equation for the Hall voltage:
Here we have a simple schematic that distills the essence of the experiment. The metallic strip with clearly labelled current (<math>I</math>), magnetic field (<math>B</math>), strip width (<math>d</math>), and hall voltage (<math>V_H</math>). Then you can relate this to the equation for the Hall voltage:


<math>V_H = \frac{1}{ne}\frac{1}{d} IB</math>
<math>V_H = \frac{1}{ne}\frac{1}{d} IB</math>,


This may be a bit over simplified -- it might be
where <math>n</math> is the carrier density and <math>e</math> is the charge.
 
Admittedly this is a bit oversimplified, but it works.

Revision as of 02:51, 8 February 2012

Schematics in reports should be straightforward and convey essential information about the experiment, including quantities (such as currents or fields) that are germane to the phenomenon under study.

Bad examples

Using the Hall Effect as an example, here are some less than useful "schematics".

The Photo of the Experiment

Unless you had done the experiment yourself, you would be left asking, "What the hall is going on in this picture?"

There is too much extraneous information here. And you can't even see the most important part of the experiment: the hall probe. Even if things were labeled, it would be difficult to make out what is what and how it does it's job. Furthermore, this does not define any key experimental quantities, like the current, the magnetic field, or the Hall voltage.

Schematic from the Manual

This is a bit better than the last, but suffers from similar problems.

More Useful

Here we have a simple schematic that distills the essence of the experiment. The metallic strip with clearly labelled current (<math>I</math>), magnetic field (<math>B</math>), strip width (<math>d</math>), and hall voltage (<math>V_H</math>). Then you can relate this to the equation for the Hall voltage:

<math>V_H = \frac{1}{ne}\frac{1}{d} IB</math>,

where <math>n</math> is the carrier density and <math>e</math> is the charge.

Admittedly this is a bit oversimplified, but it works.