In Python, objects can declare their textual representation using the __repr__
method. IPython expands on this idea and allows objects to declare other, rich representations including:
A single object can declare some or all of these representations; all are handled by IPython's display system. This Notebook shows how you can use this display system to incorporate a broad range of content into your Notebooks.
The display
function is a general purpose tool for displaying different representations of objects. Think of it as print
for these rich representations.
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from IPython.display import display
A few points:
display
on an object will send all possible representations to the Notebook.If you want to display a particular representation, there are specific functions for that:
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from IPython.display import (
display_pretty, display_html, display_jpeg,
display_png, display_json, display_latex, display_svg
)
To work with images (JPEG, PNG) use the Image
class.
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from IPython.display import Image
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i = Image(filename='images/ipython_logo.png')
Returning an Image
object from an expression will automatically display it:
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i
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Or you can pass an object with a rich representation to display
:
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display(i)
An image can also be displayed from raw data or a URL.
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Image(url='http://python.org/images/python-logo.gif')
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SVG images are also supported out of the box.
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from IPython.display import SVG
SVG(filename='images/python-logo.svg')
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Python objects can declare HTML representations that will be displayed in the Notebook. If you have some HTML you want to display, simply use the HTML
class.
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from IPython.display import HTML
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s = """<table>
<tr>
<th>Header 1</th>
<th>Header 2</th>
</tr>
<tr>
<td>row 1, cell 1</td>
<td>row 1, cell 2</td>
</tr>
<tr>
<td>row 2, cell 1</td>
<td>row 2, cell 2</td>
</tr>
</table>"""
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h = HTML(s)
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display(h)
You can also use the %%html
cell magic to accomplish the same thing.
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%%html
<table>
<tr>
<th>Header 1</th>
<th>Header 2</th>
</tr>
<tr>
<td>row 1, cell 1</td>
<td>row 1, cell 2</td>
</tr>
<tr>
<td>row 2, cell 1</td>
<td>row 2, cell 2</td>
</tr>
</table>
The Notebook also enables objects to declare a JavaScript representation. At first, this may seem odd as output is inherently visual and JavaScript is a programming language. However, this opens the door for rich output that leverages the full power of JavaScript and associated libraries such as d3.js for output.
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from IPython.display import Javascript
Pass a string of JavaScript source code to the JavaScript
object and then display it.
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js = Javascript('alert("hi")');
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display(js)
The same thing can be accomplished using the %%javascript
cell magic:
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%%javascript
alert("hi");
The IPython display system also has builtin support for the display of mathematical expressions typeset in LaTeX, which is rendered in the browser using MathJax.
You can pass raw LaTeX test as a string to the Math
object:
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from IPython.display import Math
Math(r'F(k) = \int_{-\infty}^{\infty} f(x) e^{2\pi i k} dx')
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With the Latex
class, you have to include the delimiters yourself. This allows you to use other LaTeX modes such as eqnarray
:
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from IPython.display import Latex
Latex(r"""\begin{eqnarray}
\nabla \times \vec{\mathbf{B}} -\, \frac1c\, \frac{\partial\vec{\mathbf{E}}}{\partial t} & = \frac{4\pi}{c}\vec{\mathbf{j}} \\
\nabla \cdot \vec{\mathbf{E}} & = 4 \pi \rho \\
\nabla \times \vec{\mathbf{E}}\, +\, \frac1c\, \frac{\partial\vec{\mathbf{B}}}{\partial t} & = \vec{\mathbf{0}} \\
\nabla \cdot \vec{\mathbf{B}} & = 0
\end{eqnarray}""")
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Or you can enter LaTeX directly with the %%latex
cell magic:
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%%latex
\begin{align}
\nabla \times \vec{\mathbf{B}} -\, \frac1c\, \frac{\partial\vec{\mathbf{E}}}{\partial t} & = \frac{4\pi}{c}\vec{\mathbf{j}} \\
\nabla \cdot \vec{\mathbf{E}} & = 4 \pi \rho \\
\nabla \times \vec{\mathbf{E}}\, +\, \frac1c\, \frac{\partial\vec{\mathbf{B}}}{\partial t} & = \vec{\mathbf{0}} \\
\nabla \cdot \vec{\mathbf{B}} & = 0
\end{align}
IPython makes it easy to work with sounds interactively. The Audio
display class allows you to create an audio control that is embedded in the Notebook. The interface is analogous to the interface of the Image
display class. All audio formats supported by the browser can be used. Note that no single format is presently supported in all browsers.
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from IPython.display import Audio
Audio(url="http://www.nch.com.au/acm/8k16bitpcm.wav")
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A NumPy array can be auralized automatically. The Audio
class normalizes and encodes the data and embeds the resulting audio in the Notebook.
For instance, when two sine waves with almost the same frequency are superimposed a phenomena known as beats occur. This can be auralised as follows:
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import numpy as np
max_time = 3
f1 = 220.0
f2 = 224.0
rate = 8000.0
L = 3
times = np.linspace(0,L,rate*L)
signal = np.sin(2*np.pi*f1*times) + np.sin(2*np.pi*f2*times)
Audio(data=signal, rate=rate)
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More exotic objects can also be displayed, as long as their representation supports the IPython display protocol. For example, videos hosted externally on YouTube are easy to load:
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from IPython.display import YouTubeVideo
YouTubeVideo('sjfsUzECqK0')
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Using the nascent video capabilities of modern browsers, you may also be able to display local videos. At the moment this doesn't work very well in all browsers, so it may or may not work for you; we will continue testing this and looking for ways to make it more robust.
The following cell loads a local file called animation.m4v
, encodes the raw video as base64 for http
transport, and uses the HTML5 video tag to load it. On Chrome 15 it works correctly, displaying a control bar at the bottom with a play/pause button and a location slider.
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from IPython.display import HTML
from base64 import b64encode
video = open("images/animation.m4v", "rb").read()
video_encoded = b64encode(video).decode('ascii')
video_tag = '<video controls alt="test" src="data:video/x-m4v;base64,{0}">'.format(video_encoded)
HTML(data=video_tag)
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You can even embed an entire page from another site in an iframe; for example this is today's Wikipedia page for mobile users:
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from IPython.display import IFrame
IFrame('http://ipython.org', width='100%', height=350)
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