Collimate telescope

Near the waist, the output beam best resembles an ideally collimated beam. In this region, the beam divergence is lowest, and the beam diameter stays close to the output beam waist diameter (2W'o ). But, since the beam diameter increases with distance from the waist, the extent over which the beam is considered collimated is limited. The application determines the limit, which is typically referenced to the output beam's Rayleigh range (zR'),

One of the most user-friendly aspects of USB is that its primary shape—the classic rectangle (Type-A) —is physically compatible with all earlier versions. This means USB Type-A plugs in versions 3.0, 3.1 or 3.2 will fit into old USB 2.0 ports and vice versa.

Figure 2: A 632.8 nm laser source, which has a 5 µm diameter waist (Wo) and a 31 µm Rayleigh range (zR), is collimated by a 50 mm focal length (f ) lens.

Figure 4: The input laser light better resembles a point source when it has a smaller beam waist (Wo), and therefore a shorter input Rayleigh range (zR). The collimated output beam has a Rayleigh range (zR') that depends on Wo , focal length, and wavelength. Increasing the focal length, or decreasing the wavelength, increases zR' and decreases the overall output beam divergence. The values plotted above were calculated for a 632.8 nm wavelength and a focal length of 50 mm. For comparison, values for a wavelength of 1550 nm and a focal length of 25 mm have also been calculated.

You can plug a USB 2.0 device into a USB 3.0 port and it will always work, but it will only run at the speed of the USB 2.0 technology.

Ideally, collimated light would have a constant diameter from the lens out to infinity, but no physical collimated beam maintains exactly the same diameter as it propagates. The collimated beam's divergence, which is the rate at which the beam's diameter changes, depends on the properties of both the light source and the collimator. Due to this, the collimated beam from a broadband-wavelength source, such as a lamp or light emitting diode (LED), behaves differently than the collimated beam from a narrowband-wavelength source, like a laser.

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of the collimated beam. The better the physical source resembles a single ideal point source, the lower the divergence angle of the collimated beam (Figure 1). The resemblance is closer when the physical source is very small, far away from the lens, or both.

However, where USB Type-C differs is that it’s been created purposely to take advantage of the new USB 3.1 standard. So rather than the version determining the speed and power at which data can be transferred, with USB-C it’s the connector itself.

Figure 1: If a broadband-wavelength source, like a lamp or LED, is placed one focal length (f ) away from a lens, light from each point on the source is individually collimated. The full divergence angle (θ ~ d / f ) of the output beam depends on the focal length and source diameter (d ).

As the USB standard has developed over time, it’s seen improvements in terms of speed and power, making it much quicker to run and charge USB devices and transfer data.

A Lamp or LED as a Good-Enough Point SourceA physical source adequately resembles an ideal point source when the divergence of the collimated output beam meets the application's requirements. If the divergence is too large, one option is to increase the focal length of the collimating lens, so the source can be moved farther away. However, this can have the negative effect of reducing the amount of light collected by the lens and output in the collimated beam.

Unlike LEDs and lamps, laser sources do not emit light uniformly in all directions, although the laser light's divergence can be large. If the light comes from a single-wavelength laser, there's a good chance its intensity cross section resembles a Gaussian function. The collimated beam's behavior can then be described using Gaussian beam equations, and the equations describing beam divergence would need to include the wavelength.

Collimated Laser LightThe laser source's size helps determine the properties of the collimated beam. Size is typically referenced to the beam waist radius (Wo ) or diameter (2Wo ), often through its Rayleigh range (zR),

Collimated Lamp or LED LightAn ideal point source emits light uniformly in all directions, and a positive spherical lens placed one focal length (f ) away collimates the light it collects into a beam with zero divergence. This ideal model can be adapted for use with a broadband-wavelength source, like a lamp or LED. Physical sources like these resemble groupings of multiple point sources. An adapted model for these sources takes into account the diameter (d ) of the physical light source, as well as the distance (i.e. the focal length) between the light source and the lens. The ratio of these values provides an estimate of the full divergence angle (θ ),

There are similarities between point source model adaptations for lasers and broadband sources. For example, laser sources should also be placed one focal length away from the lens to minimize the divergence of the collimated beam. In addition, the smaller the laser source (input beam waist diameter), the lower the collimated beam's divergence.

Collimatedmeaning in Physics

Anything with a version number (e.g. 2.0 or 3.0) is a standard—the technology that allows data to be transferred along a cable from one device to another.

Far from the output beam waist (>>zR'), the beam divergence is comparatively larger. The divergence in this region is reduced when the output beam waist diameter (and Rayleigh range) are increased. Here, the beam has an approximately constant full divergence angle,

By the time version 3.0 came along, USB was well established as the industry standard. In 2013 came USB 3.1, which doubled speeds to 10 Gbit/s—known as SuperSpeed+—when using USB Type A and USB-C connectors. (Read more on the different types of USB connector here.)

Collimating mirror

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in which () is the wavelength. When the input beam's waist and Rayleigh range are smaller, the collimated output beam has a lower divergence. (See Figures 2 and 3 for an example.) The divergence along the entire collimated beam can be reduced by shrinking the input source beam's waist diameter.

Yet despite being built into some of the latest hardware (newer MacBooks, for example), USB 3.1 wasn’t very widely adopted. The smartphones and other devices many people use today tend to feature USB 3.0 or earlier versions.

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Laser Point SourcesThe point source model can also be adapted for laser light, but in this case the source is defined as the input beam waist. The source size is the waist diameter (2Wo ). Typical sources include a focal spot, an optical fiber's end face, and the facet of a single-mode laser diode.

Some applications specify a distance <

So, if you plug a USB 3.0 flash drive into a USB 2.0 port, it would only run as quickly as the USB 2.0 port can transfer data and vice versa.

Collimating lens

Figure 3: The input parameters in Figure 2 create a collimated output beam with a waist located a distance one focal length (50 mm) from the lens. Note that this figure's scale is larger than the scale in Figure 2. Close to the beam waist (<>zR'), the beam's divergence can be described by a full divergence angle (). A wavelength of 632.8 nm was assumed.

Collimation radiology

Released in September 2017, USB 3.2 allows compatible devices to take advantage of the SuperSpeed (5 Gbit/s) or SuperSpeed+ (10 Gbit/s) transfer rates. However, this latest version also introduced a new SuperSpeed+ mode (20 Gbit/s) that comes into play when using a USB-C connector and the very latest models of devices.

Because USB 3.2 is still in development, it’s unlikely to be widely adopted until the industry has made its hardware fully compatible.

Launched in 2008, USB 3.0 improved significantly on its predecessor USB 2.0 by introducing SuperSpeed, a new data transfer rate that increased processing speeds more than tenfold, from 480 Mbit/s to 5 Gbit/s.

If the source waist is one focal length away from the lens, the collimated beam's waist is located one focal length away from the lens' opposite side. The beam's divergence increases with distance from the waist, and generalizations about the beam divergence can be made for regions close to and far from the waist.

A USB 2.0 cable has four wires inside it—a USB 3.0 cable has eight—and so will only transfer data at USB 2.0 speed. All components in the chain—the two devices and the cable—must be USB 3.0 to achieve that later version’s high speeds.

Here the confusion arose, as USB’s creators called its new version USB 3.1 Gen 2 (second generation), while giving USB 3.0 the new name of USB 3.1 Gen 1 (first generation).

In Figure 1, light emitted from each point on the source fills the lens' clear aperture. Rays traced from different points on the source show the output beam's diameter is smallest at the lens, and the beam appears to diverge from the clear aperture of the lens. If light from each point on the source filled only a fraction of the lens' clear aperture, the beam waist would be displaced from the lens.