Learn how to work with the notebooks by accessing the extensive information under **Help** in the navigation bar.
Learn how to work with the notebooks by accessing the extensive information under **Help** in the navigation bar.
As a first starting point you might refer to **Help>Notebook Reference**, where you can find **Notebook Examples** in the user documentation. Important basics are covered in the following sections:
As a first starting point you might refer to **Help>Notebook Reference**, where you can find **Notebook Examples** in the user documentation. Important basics are covered in the following sections:
- Notebook Basics
- Notebook Basics
- Running Code
- Running Code
- Markdown Cells
- Markdown Cells
### Python
### Python
If you need an introduction to the Python language, the **Beginners Guide** under **Help>Python Reference** links to lots of tutorials depending on your previous knowledge.
If you need an introduction to the Python language, the **Beginners Guide** under **Help>Python Reference** links to lots of tutorials depending on your previous knowledge.
### IPython
### IPython
As a more advanced user, you can benefit from the fact that Jupyter Notebooks run an **IPython** kernel, which comes with additional features with respect to the standard **Python** kernel. To learn more about these features, you can follow under **Help>IPython Reference** the link **IPython documentation** and have a look into **Tutorial>Introducing IPython**.
As a more advanced user, you can benefit from the fact that Jupyter Notebooks run an **IPython** kernel, which comes with additional features with respect to the standard **Python** kernel. To learn more about these features, you can follow under **Help>IPython Reference** the link **IPython documentation** and have a look into **Tutorial>Introducing IPython**.
The inductor in the calculation step (k + 1) can be substituted with an inductance $G_L = \frac{\Delta{t}}{2L}$ in parallel with a current source $A_L(k) = i_L(k) + \frac{\Delta{t}}{2L} v_L(k) $
The inductor in the calculation step (k + 1) can be substituted with an inductance $G_L = \frac{\Delta{t}}{2L}$ in parallel with a current source $A_L(k) = i_L(k) + \frac{\Delta{t}}{2L} v_L(k) $