X-ray Sources 101 — Micro X-Ray https://microxray.com/category/x-ray-sources-101/ Wed, 07 Feb 2024 23:39:36 +0000 en-US hourly 1 https://wordpress.org/?v=6.7.2 X-Ray Sources 101: How Long Will My X-ray Tube Last? https://microxray.com/x-ray-sources-101-how-long-will-my-x-ray-tube-last/ Wed, 07 Feb 2024 21:20:24 +0000 https://microxray.com/?p=2150 Most users of X-ray tubes intuitively understand that X-ray tube lifetime is finite, and that X-ray tubes are consumable items due to the lightbulb-like filament that is generally used as an electron source. One of the first questions when dealing with any consumable is, how long will it last? This question informs total cost of […]

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Minifocus Packaged X-ray Tube

Most users of X-ray tubes intuitively understand that X-ray tube lifetime is finite, and that X-ray tubes are consumable items due to the lightbulb-like filament that is generally used as an electron source. One of the first questions when dealing with any consumable is, how long will it last? This question informs total cost of machine ownership, preventative maintenance schedules, and a number of other key decisions needed to accurately compare one source against another.

In today’s post, we’ll look at the common failure modes of X-ray tubes, what can be done to manage them, how long your tube might be expected to last in the field, and why it’s a surprisingly hard question to answer.

A Brief Review

X-ray tubes are vacuum devices, meaning they require a high vacuum to operate. This high vacuum is needed for high voltage insulation, but it is also useful in allowing the electrons to travel from the cathode side of the X-ray tube to the anode, in order to generate X-rays. With a lower quality vacuum, the journey from cathode to anode becomes more challenging for the electrons, and therefore the filament must be run harder. For more information on this phenomenon, please see our previous articles on how X-rays are generated.

All of Micro X-Ray’s X-ray tubes are sealed type X-ray tubes. Sealed tubes are (as the name suggests) completely vacuum sealed at manufacturing, and contain no user-serviceable parts. This makes an extremely compact, robust, and durable package compared to their open type counterparts.

Filament Failure

The first failure mode to explore is failure of the filament. Modern X-ray power supplies control the beam current by tightly controlling the current through the X-ray filament. As the filament current increases, more electrons are released from the filament itself, and as more electrons are available inside the tube, more of them cross the high voltage gap to the target material, increasing the beam current. Over time, this electron emission wears down the filament, leading to an eventual end of life failure where the filament breaks completely – just like an Edison lightbulb. The lower the filament current, the longer the X-ray tube will last. The effect is a classic exponential curve – as an example, the standard 1.7A MXR filament has an estimated life of 100,000,000 hours at 1.34A, dropping to just 10,000 hours when run at the filament current limit of 1.7A. If the filament is run over the limit, say at 2.2A, it would break in a matter of seconds.

Other electron sources, for example dispenser cathodes like those used in the Microbox, have an ever longer service life than a filament-based X-ray tube.

Vacuum Degradation

Vacuum degradation is the other main cause of X-ray tube end of life. The metal components inside the X-ray tube outgas over time; this is an unavoidable law of physics, and while MXR’s X-ray tubes are built and processed with an eye towards minimizing this outgassing and improving the quality of the vacuum before sealing, the nature of sealed tubes means that not only can no gasses enter the tube, but none can escape either. As the tube heats up, the rate of outgassing internally increases.

As the vacuum degrades (meaning the pressure increases inside the X-ray tube), several things start to happen concurrently. First, the high voltage stresses inside the tube increase, which can lead to increasing leakage current, instability, and eventually arcing.

In addition to leakage increasing, the electrons from the filament have a higher change of hitting gas molecules as they traverse the high voltage gap between the anode and cathode. If an electron hits a gas molecule, it is knocked off course and loses energy, so it may not hit the target and produce an X-ray. As the vacuum degrades, therefore, the filament will need to be run hotter to compensate for those lost electrons in order to maintain a constant beam current. Over time, this process runs away, and the filament will eventually exceed its limit and open.

Race to the Death

What we have is a race to the death. As the vacuum degrades, the filament needs to work harder to keep up. As the filament works harder, the tube heats up more which causes the vacuum to degrade faster. What will happen first, will the filament run so hot it burns itself out? Or will the tube vacuum deteriorate so much that the high voltage arcs to ground, causing internal damage. There’s no one right answer, it could be either. If you’re running low kV/high current, it’s likely that the filament will burn out first. If you’re running high kV/low current, it’s likely that arcing due to vacuum degradation will occur first.

So…How Long Will my X-ray Tube Last?

10,000 hours is a good starting point for a lifetime estimate. Unless you run it hot, in which case it can be significantly less. Or, if you keep it cool, it can last longer. And of course you can’t run the filament (or cathode) too hard. If you run the filament conservatively, and keep the tube cool, it could easily last for 10x the 10,000 hour rule of thumb or more.

In practice, MXR has X-ray tubes in the field that are over 10 years old. These are usually in lab environments with a controlled atmosphere, minimal duty cycles, and adequate heating while operating. If you treat your X-ray tube well, it can last a long, long time. On the other hand, if you run 24/7 in a non-climate controlled factory in a hot part of the world, your tube just isn’t going to last as long as in the laboratory use case.

What can I do?

You can keep your tube cool! There’s not much to do about the filament other than ensure it doesn’t exceed the filament current limit, but for most tubes, the filament can live into the millions of hours before being depleted from normal operating conditions. So we’re left to focus on the outgassing, which can be minimized by keeping the tube cool. The cooler the internal components are, the slower the rate of outgassing. With a properly cooled X-ray source running within its design specifications, the lifetime of the tube can reliably exceed 10,000 hours, and often much, much more.

Contact Miro X-Ray Today

As always, let’s talk about it. Our engineers are always happy to have a conversation about YOUR application to help pick the right tube, and provide recommendations for the right cooling system.

Contact Us Today!

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X-ray Sources 101: What’s a Microfocus Source, Anyway? https://microxray.com/whats-a-microfocus-source-anyway/ Mon, 10 Apr 2023 17:48:14 +0000 https://microxray.com/?p=1955 Definition of a Microfocus Source Much to the chagrin of many in our industry, there’s no legal (or even just widely accepted) definition of a microfocus source. This leads to some understandable confusion among the X-ray source buying population, and to some occasional overly generous prose by the marketers in some X-ray source companies. In […]

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Definition of a Microfocus Source

Much to the chagrin of many in our industry, there’s no legal (or even just widely accepted) definition of a microfocus source. This leads to some understandable confusion among the X-ray source buying population, and to some occasional overly generous prose by the marketers in some X-ray source companies.

In some X-ray market segments, a microfocus is any source with a focused X-ray spot smaller than 1mm (the thinking goes, if it has a µm in front of the spot size, it’s a microfocus). Other manufacturers feel that there’s a cutoff around 100µm in order to be considered a microfocus. Still other X-ray industry pros feel that a microfocus refers to any X-ray source that’s actively focused rather than statically focused (maybe a bit too technical to be useful). There’s no right or wrong answer, it’s not like there’s an ISO definition of microfocus that’s agreed and enforceable.

So what about Micro X-Ray? We specialize in small spots, so by some of those definitions every tube we make is a microfocus tube. But when we say microfocus we generally mean any source that focuses X-rays down to under 10µm like our Microbox integrated source, and we refer to sources with larger spot sizes as Minifocus sources. Our largest spot size sources are 1000-1500µm, and in those cases we don’t generally talk about their spot sizes at all, because in the applications they’re designed for spot size isn’t an important specification point. If you need a refresher on what exactly we mean when we’re talking about focal spot, then check out our post on the topic in the Resources section of our website.


Spot Sizes in Imaging

Imaging applications are generally all about identifying features hidden inside opaque materials. Whether you’re imaging a rock, a pebble, or a grain of sand, you can use X-rays to see inside them all. X-rays have the ability to penetrate objects that visible light cannot, which makes them incredibly valuable in a huge array of application spaces from security to food inspection to electronics manufacturing. With X-ray sources, there are three main knobs you can turn that impact the final image:

  1. Excitation voltage: This sets the maximum penetration ability of the X-rays. The higher the voltage, the higher density object you are able to image.
  2. Beam current: This sets the absolute number of X-rays from the source. The higher the beam current, the more X-rays. The more X-rays, the faster an image can be acquired, and the faster your product can be moved through the process.
  3. Spot size: This sets the minimum feature size able to be imaged in an X-ray system. The smaller the spot size, the smaller the size of the feature that can be resolved on the X-ray image

If we think about these three knobs, you can start to map them on to your application and narrow down your X-ray source options. If you have a general idea of the density of the object to be scanned, the process time you have available to scan it, and the size of the features you’ll need to resolve, you have a great starting point for selecting an X-ray source. Of course, there are always tradeoffs, so you might choose a slightly higher resolution that takes a slightly longer time, or perhaps the ability to have a quick process time might come at the expense of slightly lower contrast on dense materials. Either way, once you have your application properly scoped, at a great point to reach out to our technical team so we can find the right source together.


Spot Sizes in Analysis

Most analysis applications couldn’t care less about spot size. Take X-ray attenuation thickness gauging, for instance. This application works by passing a thin film of some known material between an X-ray source and an X-ray detector. The system is calibrated with the tube and detector a fixed distance apart, and the total flux from the X-ray tube is empirically measured and stored. Because the material is known, the absorption of the material for a given X-ray energy can be calculated. During operation, the X-ray flux is read back continuously from the detector, and the thickness can be calculated with a high degree of precision based solely on the attenuation of the X-ray beam through the film. At no point in this process is the spot size of the X-ray tube impactful, and for this reason the majority of thickness gauging applications tend to use tubes with our largest spot sizes, around 1000um.

Of course, not all X-ray analysis applications are created equally, and for some (I’m looking at you, µXRF) the spot size is critically important. But in general, spot size usually only matters for imaging applications.


Summary

The definition of a microfocus source matters much less than selecting the right spot for you application. If you’re in the market for an X-ray source of any kind, it’s best to understand your application and select a source with the spot size you need, and understand that terms like microfocus, small spot, etc are really all just marketing terms with no standardized definition. The spot size YOU need depends on YOUR use case. We here at Micro X-Ray are always happy to discuss your applications, and get you the right tube for your application, whether you need a 5µm spot, a 1500µm spot, or something in between.

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X-ray Sources 101: Bremsstrahlung Radiation and Why it Matters for Imaging https://microxray.com/x-ray-sources-101-bremsstrahlung-radiation-and-why-it-matters-for-imaging/ Wed, 05 Apr 2023 15:47:29 +0000 https://microxray.com/?p=1947 We’ve talked before about choosing a target material, what a spectrum looks like, and why it matters for analytical applications. Many imaging applications overlook the importance of their tube’s spectrum and how it impacts image contrast and quality. Today we’re going to look specifically at bremsstrahlung radiation, learn what it is and why it matters […]

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We’ve talked before about choosing a target material, what a spectrum looks like, and why it matters for analytical applications. Many imaging applications overlook the importance of their tube’s spectrum and how it impacts image contrast and quality. Today we’re going to look specifically at bremsstrahlung radiation, learn what it is and why it matters in X-ray imaging.


Physics of Bremsstrahlung Radiation

Bremsstrahlung radiation, also known as “braking radiation,” is a type of electromagnetic radiation produced by the deceleration of charged particles, such as electrons, when they pass through the electric field of an atom in an X-ray tube’s target. In X-ray tubes, the charged particles, or electrons, are accelerated by a high voltage, usually in the range of 20 to 150 kV, and then collide with a target material, such as tungsten. These collisions result in the deceleration of the electrons, and the energy lost by the electrons is emitted as Bremsstrahlung radiation.

Briefly, Bremsstrahlung is different than characteristic radiation which is produced when one of the same electrons knocks an electron from an inner shell out of orbit. An electron from a higher shell jumps down to fill the gap, and the difference in energy between the shells is emitted as an X-ray. The energy of that X-ray is equal to the energy difference between the two shells.

The energy of the Bremsstrahlung radiation is directly related to the energy of the electrons, as well as the atomic number of the target material. The higher the energy of the electrons, the higher the energy of the emitted Bremsstrahlung radiation. Similarly, the higher the atomic number of the target material, the higher overall count rate of the emitted Bremsstrahlung radiation.


X-ray Imaging

Bremsstrahlung radiation is significant in X-ray imaging because it is the primary source of X-rays in X-ray tubes. The X-rays produced by Bremsstrahlung radiation are favorable for imaging purposes because they have a broad spectrum of energies, allowing for higher contrast images in materials with varying densities. This broad spectrum of energies is due to the fact that the electrons that produce the X-rays lose different amounts of energy as they pass through the target material, resulting in a wide range of X-ray energies.

The upper limit of the X-ray tube’s energy output is set by the excitation voltage of the source, and the lower limit is set by the inherent filtration of the tube, in the example below we see both the Bremsstrahlung generated at the target face, along with the output of the X-ray tube with the 254μm Be window’s inherent filtration taken into consideration.

Bremsstrahlung output of an X-ray tube
Generated Bremsstrahlung of an X-ray tube, and the same tube’s output filtered by a 254μm Be window

The voltage applied to the X-ray tube and the choice of additional filtering materials are carefully chosen to produce X-rays with the desired energy spectrum for a given imaging sample. Often in imaging applications, the characteristic lines of the target material are filtered out to ensure a clean Bremsstrahlung radiation pattern for optimal imaging of the widest possible array of samples.


Summary

Bremsstrahlung radiation is a type of electromagnetic radiation produced by the deceleration of charged particles, such as electrons, when they pass through the electric field of a heavy atom in an X-ray tube. It is the primary source of X-rays in X-ray tubes and plays a crucial role in X-ray imaging. By understanding the generation and properties of Bremsstrahlung radiation, we can better understand the workings of X-ray tubes and their applications in medical and industrial imaging.

If you have any questions about target materials, imaging applications, or X-rays in general, don’t hesitate to reach out to us today!

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X-ray Sources 101: Taking Faster Images at Higher Resolution (Part 2) https://microxray.com/x-ray-sources-101-taking-faster-images-at-higher-resolution-part-2/ Wed, 01 Mar 2023 19:55:12 +0000 https://microxray.com/?p=1892 Before jumping into today’s post discussing Micro X-Ray’s unique diamond anode and how it can speed up your imaging applications, here’s a little background reading: Part 1 of this series Our article on voltage, current, and power Our article on spot size In Part 1, we followed the path of an X-ray from generation inside […]

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Before jumping into today’s post discussing Micro X-Ray’s unique diamond anode and how it can speed up your imaging applications, here’s a little background reading:
In Part 1, we followed the path of an X-ray from generation inside the tube through detection on a single pixel of an X-ray detector. We discussed the probabilities around the X-ray making it to the detector, and we learned that if you increase the amount of X-rays generated, then you decrease the time required to take an X-ray image.
So, what if you want to halve the image acquisition time? It should be as easy as turning up the power, right? As with all X-ray questions, the answer is yes, but…

Power Loading

In this case, the “but” is power loading causing damage to the target. The smaller the spot size, the tighter the concentration of power within the target disk. If you’ve ever played with a magnifying glass in the summer, you’ll already be familiar with this concept.
Magnifying glass concentrating the sun's rays onto a sheet of paper
A magnifying glass focuses the sun’s rays which are otherwise evenly spread over the diameter of the glass and, when held at the right distance from the ground, focuses those rays down to a very small and bright focal spot. Those same rays that were spread out evenly over the diameter of the magnifying glass which may have caused a minor sunburn after a half hour or so, when concentrated into a small focal spot now have the potential to start fires and melt crayons within seconds. You can adjust the focal spot of the magnifying glass to create a very small and bright spot, or a less small and less bright spot by changing the geometric optics (moving the magnifying glass up and down in space).
Similarly, the power in the electron beam, is concentrated using electrostatic optics into a focal spot on the X-ray tube’s anode. The power of the electron beam is given in W, and the focal spot size is given in microns. We can divide the two to get a power loading factor expressed in Watts per micron (W/μm). This can be thought of as the “brightness” of the spot. If you increase the beam power but keep the spot size constant, the brightness increases. Similarly, if you decrease the spot size but keep the power constant, you will also increase the brightness. So why not just make an infinitely small spot with as much power as your detector can handle?

Target Material Selection

Comparison of pitted and non-pitted target spots

X-ray spot visualization of an undamaged target (left), and a pitted target (right)

Depending on the properties of the target material, the target face can handle more or less power before failure. When a target fails, or becomes pitted, the intensity of the spot damages the target material and burns a hole through the target disk down to the anode substrate, which has the effect of reducing the flux intensity in the spot to a fraction of its value. The image above shows a undamaged target and a pitted target on the same scale – notice that the spot intensity in the center of the undamaged target’s spot actually exceeds the detector’s 16k counts, while the pitted target has a maximum intensity of under 6k counts. This is because the center, brightest point in the spot has burned through the target disk and is no longer producing X-rays.
Thinking back to our magnifying glass example, the same focal spot size under the magnifying glass can burn skin, cause paper to combust, and cause absolutely no damage to concrete. The difference isn’t the power in the focal spot, it’s the durability of the material the focal spot is concentrated on.
Different X-ray target materials all have different properties. Tungsten (W) is a common X-ray target because it not only produces a nice clean Bremsstrahlung radiation profile, but it also happens to be a quite durable metal with a high melting point. Conversely, Gold (Au) produces very useful peaks in certain XRF applications, but it is such a soft metal that a relatively dim focal spot (ie, low power loading) will cause damage to the target material, resulting in such low achievable count rates as to negate its benefits in all but the most specialized of applications.
Because W is the common choice of target material for imaging applications, we’ll focus on W target sources. A safe rule of thumb for power loading on a standard W target X-ray tube is 1W/μm. Beyond 1W/μm, the spot will generate too much power for the target to handle, and the target disk will be damaged, sometimes in a matter of seconds. Micro X-Ray has developed a unique target material structure using a Diamond substrate to move the heat out of the spot and into the anode much more efficiently than a standard target structure. This allows us to run at a 50% increase in power loading compared to a non-Diamond backed target, allowing for a 1.5W/μm power loading number.

Higher Power Loading Enabling Faster Images

What does this all mean? If we remember from Part 1, the more photons you have hitting your detector, the faster you can get an image. If you need, for example, 10 million photons to hit your detector, you can get there 50% faster by increasing the power by 50%. And with our diamond target, you can do just that, and accumulate your 10 million counts faster to increase your line speed.
Alternatively, what if you have a fixed amount of time in your process in order to take an image? Our Diamond target can help there, too, by allowing you to reduce the focal spot size while keeping the power consistent. This will result in a higher resolution image in your defined process time.

Micro X-Ray Diamond Anode Products

Both our Microbox integrated X-ray source and our Seeray water-cooled X-ray tube contain our unique Tungsten/diamond anode technology.

Graph showing the Microbox maximum power operation

Microbox Operating Range, Maximum Power

 

Graph showing the Microbox Minimum Spot Size Operation

Microbox Operating Range, Minimum Spot Size

In the case of the Microbox, this allows us to run at an industry-leading power loading of 1.5W/μm, enabling faster and crisper images than our competitors. Whether you’re interested in maximizing the power at a given spot size, or maximizing the resolution in a given exposure time, the Microbox’s 1.5W/μm power loading will give you measurable improvements against any other Microfocus source on the market.
Seeray X-ray Tube
In the case of the Seeray, our diamond anode technology is coupled with a unique direct water-cooled anode. This allows for the same 1.5W/μm power loading as the Microbox source, while the direct anode cooling allows for beam powers of 100W or more. The direct anode cooling also enables super-fast beam stabilization times, making this an ideal tube for X-ray optic coupling and single crystal XRD.

For More Information on Diamond Anodes

We’re always available to talk about X-rays, and help you weigh the tradeoffs and consider the various application constraints to pick the right source for you. Reach out to us today to talk about how our diamond anode technology can be put to use to optimize your X-ray application today!

Contact Us Today!

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X-ray Sources 101: How to Choose a Target Material for XRF https://microxray.com/x-ray-sources-101-how-to-choose-a-target-material-for-xrf/ Tue, 20 Dec 2022 17:10:06 +0000 https://microxray.com/?p=1833 Target Material for XRF Instruments Selecting the appropriate anode target material for XRF (X-ray fluorescence) instruments is critical for obtaining precise and dependable results. The X-ray tube is the heart of the XRF equipment, and the target material inside the X-ray tube determines the primary spectrum of X-rays emitted. Different target materials possess unique properties, […]

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Target Material for XRF Instruments
Selecting the appropriate anode target material for XRF (X-ray fluorescence) instruments is critical for obtaining precise and dependable results. The X-ray tube is the heart of the XRF equipment, and the target material inside the X-ray tube determines the primary spectrum of X-rays emitted. Different target materials possess unique properties, and choosing the appropriate material can help you reduce measurement time, obtain more precise results, and generally optimize your XRF calculations.

Elements to be Measured

The first question in any XRF system design is: what are you looking for? There many different applications for XRF: some XRF machines are designed to quickly sort between different scrap metals, some are designed to quantify trace amount of Sulphur in crude oil, some are designed to analyze coating purity and thickness over various substrates, and some are general purpose machines which need to be robust enough to be able to identify nearly any element within a wide range of atomic numbers. Understanding the materials to be measured, the minimum detection limits of those materials, and the time allocated for measurement are crucial to selecting the right X-ray tube and target.

Primary X-ray Spectrum

The target material, when bombarded with electrons, creates the primary X-ray beam. That beam is then directed at the material under test, which generates a secondary X-ray beam. It is the that secondary beam whose spectra is captured by the X-ray detector and analyzed.
The spectrum created by this beam is a function of the target material and the energy of the electrons in the beam (set by the Excitation Voltage). The X-ray spectrum is made of up two components: the bremsstrahlung background radiation, and characteristic peaks fluoresced by the target material.
Depending on the characteristic peaks of the elements that are being resolved, the specific characteristic peaks of a material such as Rh or Ag may be beneficial. For more general XRF applications which are relying on long measurement times to resolve unknown materials, a W target with a large bremsstrahlung and minimal characteristic peaks may be beneficial.

Lightbright Spectra

Spectra from two different Lightbright tubes at 50kV with different target materials

In the chart above, we can see spectra from two different X-ray tubes with different target materials. These are same X-ray tube type, run at the same excitation voltage (50kV), the same beam current, and the same acquisition time, and the same detection system. Neither spectrum is inherently better or more useful for XRF than the other; depending on the elements we are trying to analyze, the peaks around 20keV in the orange spectrum may be useful, or in other cases the higher bremsstrahlung shown in the blue spectrum may be more beneficial.

Power Requirements & Target Durability

Faster measurement times can be enabled with higher flux. For any given target material, an increase in beam current will lead directly to an increase in flux. A high power application, or an application with a particularly demanding thermal environment, may require a relatively more durable X-ray target to ensure a long service life. The characteristic lines of Au, for instance, are very helpful in resolving certain elements. However, Au is notoriously soft, and the power of the X-ray spot can easily damage the target disk, resulting in an unusable X-ray tube. Therefore, Au target tubes are rare, and only deployed in very specific applications with very specific requirements.
By contrast, a W target may have fewer useful characteristic peaks for XRF, but its durability means that it can withstand much higher power loading than a comparable spot size Au target. Therefore, in some applications it may be more suitable to select a W target tube with a robust bremsstrahlung and lower characteristic peaks with a higher power rating compared with an Au target tube with specific characteristic peaks but with a lower overall power rating.

Conclusion

In summary, selecting the appropriate anode target material for XRF instruments is essential for obtaining precise and reliable results. Before making your selection, it is important to understand the tradeoffs between the available options.
Micro X-Ray manufactures end window and side window tubes optimized for XRF with Rh, W, Mo, Ag, Au, Cr, Co, and other targets. We’re always happy to talk through the pros and cons of each target material given your unique XRF requirements. Please reach out today!
Contact Us Today!

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X-ray Sources 101: Voltage, Current, and Power in X-ray Tubes https://microxray.com/x-ray-sources-101-voltage-current-and-power-in-x-ray-tubes/ Tue, 06 Dec 2022 17:03:15 +0000 https://microxray.com/?p=1806 Introduction X-ray tube power is defined as the product of beam current and excitation voltage. X-ray tubes work by accelerating electrons across a gap between a low voltage potential and a high voltage potential. As we learned in the article about X-ray Tube Topologies, there are several different ways to generate the required voltage. In […]

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Power = Voltage x Current


Introduction

X-ray tube power is defined as the product of beam current and excitation voltage. X-ray tubes work by accelerating electrons across a gap between a low voltage potential and a high voltage potential. As we learned in the article about X-ray Tube Topologies, there are several different ways to generate the required voltage. In this app note, we’ll assume we’re working with a positive polarity X-ray tube, meaning the electrons start at the cathode near GND potential and are accelerated towards a positive high voltage target on the anode. Three key specifications are important in picking an X-ray power supply and designing the electrical system to power your X-ray tube: excitation voltage, beam current, and tube power. A dedicated X-ray power supply (either integrated or stand-alone) is required to operate a tube, and an understanding of these three key variables and their interrelationship is crucial to selecting the right power supply.

Excitation Voltage

Excitation voltage is the potential difference between the cathode side of the tube and the anode side of the tube. This voltage sets the highest energy X-ray (in keV) that the X-ray tube is able to produce. The exact spectrum of X-rays generated by the tube is determined by a combination of the characteristic peaks of the target material and the Bremsstrahlung radiation produced by all X-ray tubes. X-ray tubes generally operate in the kV range, with a typical excitation voltage of around 50kV in analytical applications, and 100kV+ in imaging applications. MXR produces a range of tubes that can operate with excitation voltages of 4kV to over 100kV.

Beam Current

This is a count of the number of electrons moving from the cathode side to the anode side across the gap.
The electron source can be controlled to increase or decrease the amount of electrons emitted, thus controlling the beam current of the tube.
The more electrons are travelling across the gap, the more X-ray flux is generated when the electrons slam into the target material. As the beam current increases, the X-ray flux increases along with it. Micro X-Ray‘s X-ray tubes operate in the microamp (μA) and milliamp (mA) ranges.

Tube Power

In an electrical system power is defined as P=V×I, and X-ray tubes are no different. In the case of X-ray tubes, the tube power is defined as the excitation voltage times the beam current. X-ray tubes are highly inefficient machines, meaning that the majority of the power used is converted to heat, with only a small fraction of the total power being converted to useful X-rays. From an application standpoint, this means that the higher your system power, the more heat management will need to be designed into your machine.

X-ray Power Supplies

When selecting an X-ray tube power supply, it is important to understand all three of these values. For example, some X-ray power supplies may provide 50W and 10mA, but they can only do so at 5kV. If you need 50kV X-rays, then this power supply will not be suitable.
Another power supply may provide 50kV and 100W, but will have a 2mA maximum beam current limitation. While this is suitable for 50kV operation (50kV × 2mA = 100W), you will be limited to 60W maximum if you run the supply at 30kV (30kV × 2mA = 60W).

We’re always available to help you select the right tube AND power supply for your application. Contact us today to learn more about our X-ray tube, source, and power supply offerings!

Contact Us Today!

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X-Ray Sources 101: What is Focal Spot Size and Why Does it Matter? https://microxray.com/x-ray-sources-101-what-is-spot-size-and-why-does-it-matter/ Tue, 22 Nov 2022 16:59:52 +0000 https://microxray.com/?p=1711 In simple terms, the focal spot size is the size of the electron beam where it hits the target on the tube’s anode. For most analytical applications like XRF, the focal spot size doesn’t really matter (there are always exceptions, of course). As long as the focal spot is “reasonably” small and stable, it is […]

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In simple terms, the focal spot size is the size of the electron beam where it hits the target on the tube’s anode. For most analytical applications like XRF, the focal spot size doesn’t really matter (there are always exceptions, of course). As long as the focal spot is “reasonably” small and stable, it is not too important of a spec point. Spot size is a key spec point in any imaging application, so that’s where we’ll focus today.

Spot Size and Resolution

In an imaging application, the focal spot size of the source you’re using is going to be a major factor in the resolution of the image you’ll eventually get out of the source. To understand this, let’s first think of shadows cast in visible light. If you hold an object in front of a normal incandescent bulb, the shadow it creates will have soft edges due to the diffuse surface area of visible light being emitted from the light bulb’s filament. If you hold the same object in front of an LED (say, your phone’s flashlight) the resulting image will have noticeably crisper, sharper edges. This is because the light emitted from the LED is emitted only from the diode’s PN junction and expanding outward from there. In fact, in LEDs this is often a problem as people are adverse to overly-crisp shadows in their homes and offices. As a result, many LEDs incorporate some optical element or opaque plastic in order to diffuse the light to more closely mimic the incandescent style shadows we’re accustomed to.
Now let’s apply the same thinking to X-rays. Unlike photons of visible light, X-ray photons have the ability to penetrate optically opaque materials, so an X-ray image is really just a shadow of the density of the inner components of an object. The same principles that dictate the sharpness of a shadow in visible light hold true in X-rays as well. A smaller X-ray focal spot size correlates to the smaller emission area of an LED, so we can expect sharper, crisper X-ray images with a smaller focal spot size.

Image Quality

There are a few terms to define here that relate to the X-ray image quality:
  • Geometric Unsharpness: The quantitative term for the loss of definition in an image due to focal spot size (and other geometric factors).
  • Penumbra: The partially shaded region on the edge of the shadow in an image.
Let’s look at some examples to help clarify these terms. We’ll look at the penumbra generated by an ideal X-say point source, where all X-rays are generated in the exact same space. Then we’ll look at the X-rays generated by a focal spot of a Microfocus tube with an X-ray spot of 5μm.

x-ray point source

X-ray coverage on a detector shown with a X-ray point source

In this first image, the X-rays are emitted from an ideal point source. In this case, the penumbra (illustrated by the thin red line on the edge of the X-ray image on the detector) is nearly nonexistent.

x-ray spot source

X-ray coverage on a detector shown with a X-ray spot of some quantifiable size

In this second image, the X-rays are generated in a focal spot with some real diameter, not an ideal point source. In this case, we can see the penumbra is quite a bit larger than with the point source. This is due to the fact that X-rays from all areas of the spot are hitting the edge of the object at slightly different angles, causing partial shading in the detector image.
Armed with this information, we can see that the highest resolution object you can image, therefore, will be dictated by the size of the spot.

What does this mean in practice?

When selecting a spot size, the amount of geometric unsharpness that you can tolerate depends on the size of the feature you’re measuring and the size of the penumbra.

 

Line Pair Gauge

X-ray image of a line pair resolution gauge, with line pairs from 3 – 30 microns.

The above image is of an X-ray of a line pair gauge, taken with a Microbox with a 5μm focal spot size. The line pairs are a high density material on a low density substrate. Each grouping is a set of three lines of a certain width, spaced the same width apart. This gives us a easy, repeatable way to measure the size of resolvable details using any given X-ray source.

3D visualization of 5µm line pairs

Visualization of 5µm line pairs with the grey value assigned to the Z axis.

If we now zoom in on the 5µm line pair and apply a 3D visualization by assigning the grey value to the Z axis, we can easily resolve the three distinct peaks by eye; one peak for each of the three 5um width lines on the gauge. However, notice the pyramidal shape and how the features tend to blur together at the base of the shape. This is the penumbra from the 5μm spot causing geometric unsharpness that’s blurring the image, and because the lines and spaces are themselves only 5μm, we are nearing the minimum resolvable feature size of this source. Whether or not this resolution is good enough is a choice for the system designer to make.

30µm line pair

Visualization of 30µm line pairs with the grey value assigned to the Z axis.

Next, we’ll zoom in on the 30µm pair from the same line pair image, and apply the same 3D visualization. In this case we can see a distinct tabletop shape to the lines, with a clear valley between them. This is because the penumbra from a 5µm spot will only blur the outer 5µm of the lines. Because the lines are 30µm wide and the space between them is 30µm wide, the line pairs are clearly resolvable and can easily be distinguished.


What size spot do you need?

As with everything in X-rays, it depends. If your application is an online QC process on canned food and you need to see things like bone fragments left in processed meats, you generally won’t need to see anything less than about 500μm. If you’re looking at bond wires inside an integrated circuit package, you may need to see if a 12μm bond wire is intact and correctly spot welded to the die. Spot size, feature size, magnification, and more all play a part in determining the ideal spot size for any application.
Because X-ray sources tend to increase in complexity (and cost) as the spot size decreases, it is important to understand the minimum size object you need to resolve, and work backwards from there to identify the correct X-ray source. The MXR support team is always available to help guide these conversations to the best tube for your application.

Other factors affecting resolution

Of course, the detector is going to play a large part in this as well. A flat panel detector behaves differently than an image intensifier. An energy discriminating detector is going to not only give you a photon count, but also a photon energy reading. A detector with a 100um pixel pitch might work for some high magnification applications, but render your image completely useless in other applications.
In addition to the spot size and the detector used, careful attention must be paid to the geometry of the system, the cone angle of the tube, and the mechanical stability of the system. In some systems, a tiny vibration from, say, an automated stage will render your images useless for a CT reconstruction algorithm, but will be perfectly acceptable for a 2D fluoroscopy application.

Let’s Talk!

Contact us today to talk about your imaging application, our Microbox source which is purpose-built for X-ray imaging, or anything else X-ray related!

Contact Us Today!

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X-ray Sources 101: X-ray Tube Topologies https://microxray.com/x-ray-sources-101-x-ray-tube-topologies/ Wed, 26 Oct 2022 16:56:50 +0000 https://microxray.com/?p=1678 What are X-ray tube topologies? The topology of an X-ray tube refers to how the excitation voltage is generated inside the high voltage power supply. Determining which of the several common X-ray tube topologies is suitable for a high voltage supply is one of the first design decisions to make in any X-ray application. An […]

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What are X-ray tube topologies?
The topology of an X-ray tube refers to how the excitation voltage is generated inside the high voltage power supply. Determining which of the several common X-ray tube topologies is suitable for a high voltage supply is one of the first design decisions to make in any X-ray application.
An X-ray tube anode always has a high excitation voltage relative to the X-ray tube cathode. This is required so the electrons emitted from the electron gun see a large positive potential difference and accelerate towards the anode. Without this positive high voltage difference, X-ray generation would not be possible.
The most straightforward method is to put a high voltage supply on the tube’s anode, and a ground-referenced low voltage supply on the tube’s cathode. However, this is not the only way! Below, we’ll review three of the most common X-ray tube topologies.

 


Grounded Cathode Topology

Grounded Cathode X-ray Topology
This is the most common of MXR’s tube topologies. A grounded cathode means the cathode end of the tube is referenced to ground. In the case of a filament tube, this means one end of the filament is at the ground potential, and the other end is just a few volts higher. This makes for a simple filament control loop, which can be achieved with low voltage cables and (relatively) simple power supplies.

Grounded Anode Topology

Grounded Anode X-ray Topology
This topology is the opposite of the grounded cathode. In this case, the anode side of the X-ray tube is referenced to ground, while the cathode side is referenced to (floats on top of) a negative high voltage. The voltage difference of the anode with respect to the cathode remains the same. This topology is useful in certain cases where reducing the focal spot to object distance (FOD) to the absolute minimum is required, as it allows the target to be moved extremely close to the X-ray window without worrying about high voltage fields near the grounded window. However, the floating filament supply requires relatively complex circuitry to monitor and control because it is floating many thousands of volts below the ground potential.

Bipolar Topology

Bipolar X-ray Topology
A bipolar topology contains both a floating cathode and a floating anode. The advantage to this topology is that it allows you to use dual smaller, lower voltage supplies in order to achieve the same excitation voltage as a larger, higher voltage supply. For example, if your X-ray tube is designed for an 80kV excitation voltage, a bipolar supply will achieve this with dual 40kV supplies, one positive polarity and one negative polarity.  This is advantageous because the creepage and clearance requirements on a single +80kV supply are much larger than on dual +/-40kV supplies.

Contact us today to learn more about our X-ray tube, source, and power supply offerings!

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X-ray Sources 101: Anatomy of an X-ray Tube https://microxray.com/x-ray-sources-101-anatomy-of-an-x-ray-tube/ Thu, 15 Sep 2022 15:17:01 +0000 https://microxray.com/?p=1478 What are the major parts of an X-ray tube? X-ray tubes come in many different shapes, sizes, materials, and configurations depending on their ultimate end application, but all X-ray tubes share some common anatomy. In the analysis space, there are tubes specialized for X-ray Fluorescence, X-ray Diffraction, and online process control of all kinds. There […]

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What are the major parts of an X-ray tube?

X-ray tubes come in many different shapes, sizes, materials, and configurations depending on their ultimate end application, but all X-ray tubes share some common anatomy. In the analysis space, there are tubes specialized for X-ray Fluorescence, X-ray Diffraction, and online process control of all kinds. There are also tubes for many different kinds of imaging applications, from checking bond wires inside electronic components to looking at recently biopsied tissue samples to verifying fill levels in opaque canned and bottled goods. Every tube MXR makes is tailored to your specific end application, but the building blocks of the tubes are universal. In this edition of X-ray Sources 101, we’ll look at the parts of an X-ray tube that you’ll find, no matter the application.

X-ray Tube Parts: Cathode

All X-ray tubes need a source of electrons, and this can be found on the cathode side of the tube.  Cathode side configuration will vary from tube to tube, but will always include an electron source and some sort of focusing elements. In the case of the most simple filament tube, the cathode side consists of just a filament and passive focusing cup at the ground potential. At the other extreme, the cathode may contain a cathode emitter, beam shields, and several focusing grids at various voltages to assist with electron extraction and beam shaping.

X-ray Tube Parts: Anode

Just as all X-ray tubes need an electron source, they also need a target for those electrons to hit. Most MXR sources use reflection-style anodes, which are a combination of a thin target material disk and copper heatsink. There are a variety of different target materials that produce different X-ray spectra (we’ll cover the topic in a later issue), but in principle X-rays are created in the same way regardless of target material (that mechanism, too, will be the topic of a later issue). The target disk is generally bonded to a large piece of copper which acts to remove the heat generated in the spot and direct it away from the target material.

X-ray Tube Parts: Window

A window is where the useful X-rays exit the tube. An individual X-ray is emitted in a random direction based on the interaction between the electron beam and the target material electron that it collides with. X-rays are generated in a spherical pattern around the target, with half of the sphere being directed back into the target material, and half of the sphere extending outwards from the target material. Some amount of the X-rays generated are directed towards the X-ray tube’s window. Beryllium is a desirable window material due to its position as the lowest Z metal, allowing for a tight vacuum seal, mechanical robustness, and minimal X-ray attenuation. In some cases  other materials may be used where the attenuation of low energy flux due to the window is not important.

About Micro X-Ray

Micro X-Ray designs and manufactures X-ray tubes and X-ray sources entirely in our California facility. Our X-ray sources provide best-in-class performance for a wide variety of applications. We offer packaged tubes in various configurations and geometries, with customizable power levels, target materials, spot geometries, integrated shielding, and integrated cooling options tailored to your application and environment. Whether you are a large OEM, system integrator, repair facility, or university, we welcome the opportunity to discuss your specific X-ray tube requirements.

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X-ray Sources 101: X-ray Tube Grounding Considerations https://microxray.com/not-all-grounds-are-the-same/ Mon, 12 Sep 2022 18:01:32 +0000 https://microxray.com/?p=1360 X-ray Tube Grounding and Instability When evaluating and using an X-ray tube, it is important to pay attention to the X-ray tube grounding topology. An improper ground path, a loose ground connection, or a mismanaged high voltage return line can result in tube instability that is tricky to diagnose. Recently, we have had a customers […]

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X-ray Tube Grounding and Instability

When evaluating and using an X-ray tube, it is important to pay attention to the X-ray tube grounding topology. An improper ground path, a loose ground connection, or a mismanaged high voltage return line can result in tube instability that is tricky to diagnose. Recently, we have had a customers call us with an X-ray tube stability issue. They had recently received our X-ray tubes and installed them in their systems to begin testing. We then received notice that there was something wrong with the stability of the tube.

Our tubes are thoroughly tested before they leave our factory to ensure they are plug-and-play ready. Improper grounding is one of the leading causes of instability and can typically be characterized in one of two scenarios:

High Voltage Grounding Connection  

Some customers choose to perform quick tests after receiving the unit as a form of incoming inspection. Even (or especially) when doing a ‘quick test’, care needs to be taken!

Using temporary grounding connections is a sure-fire way of causing instability, or worse, damage! Temporary grounding simply cannot manage the high voltage (HV) it needs to dissipate. Whenever voltages over 600V are being used, proper grounding is a necessity. That means adequate cable sizing (min 12 AWG or larger) with a suitably sized ring or spade connection. Never use an alligator clip to ground any HV circuit!

Earth Ground

This is a ground physically and electrically connected to Earth via a conductive material. Although it seems natural to ground to the nearest bolt or screw, care needs to be taken to make sure that whatever you are connecting to has a suitably low inductance path directly to Earth.

One of the most common causes of tube instability is caused by a floating ground. This occurs when not all grounds are suitably connected to the same earth ground. A floating ground can quickly cause the tube to become unstable and lead to arcing. A ground which seems suitable at a low kV setting may suddenly appear to be failing at higher kV settings. Once the ground path is compromised, arcing in the tube begins to deplete the vacuum, which causes the premature end of filament life.

Test and Verification

It is always a good idea to put a high quality ohmmeter across all ground connections to make sure there is a dead short between them. If these poor grounding conditions exist, then damage to the X-ray tube may occur.

At Micro X-Ray, we put a lot of emphasis on building high-quality and high-performing X-Ray tubes and integrated solutions. The last thing we want is a tube to be damaged from something as simple as an improper ground connection.

Contact us today with your questions about grounding, or to learn more about our X-ray tube options and why we should be your top choice.

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