Chiropractic offices have traditionally kept pace with other medical practices in their use of technology. From patient records to billing, many chiropractors are better managing patient care, thanks to evolving technology.  More and more technological advancements are making their way into chiropractic practices. Today’s technology is not only streamlining chiropractic office administration, it’s arming these practices with better diagnostic tools. 

Weigh Costs vs. Savings

Switching from traditional X-ray films to a digital or computed radiography (CR) scanning system whose advantages are vast may seem enticing, but the bottom line questions are still, “Is such a system affordable for my practice?  Will the benefits outweigh the costs; and how long before I can recoup my investment in a digital system?”

Prices are coming way down and that has helped make the up-front investment more affordable for more and more chiropractors.  The new systems are suitably sized and priced for the private office.  That fact, combined with the long-term savings to be realized from the elimination of disposables such as film and chemicals, as well as freedom from frequent maintenance and waste disposal, makes the transition to digital an attractive proposition worth serious consideration.

In addition to doing away with X-ray film, costly chemicals, hazardous chemical disposal and film processor maintenance and repairs, digital imaging eliminates the need for sizeable film storage facilities and a dedicated darkroom.  The space savings alone provides a valuable advantage, allowing you to reclaim precious room that can be utilized for patient care.  The annual savings for a practice that takes as few as eight films a day can be as high as or even higher than $9,000 after switching to digital.

So, where does that leave you on the cost side of the equation?  Until very recently, digital and computed radiography imaging systems were priced well out of the reach of the average chiropractic office.  Today, however, there are a number of companies offering these systems that provide all of these advantages at a much more reasonable price.

Realistically, you are looking at an investment of between $32,000 and $40,000 for a computed radiography scanning system.  So, if you are taking eight or more films a day and saving approximately $9,000 every year (see chart), that means that, over the course of four to five years, you will have paid for the system with the savings.  From that point forward, you can start banking the savings. Obviously, a practice that is doing a larger number of daily X-rays would reach a breakeven point more quickly and recoup the cost of the system faster.

How Does CR Work?

The CR processor uses a special re-useable imaging plate containing photosensitive storage phosphors that retain the image until it is sent to the computer. These plates can be reused thousands of times before being replaced. X-rays are taken in the usual manner. The plate is then removed from its cassette, inserted into a scanner where the image is scanned, and automatically transferred to your computer in less than a minute. You’ll know right away if you need to take another view, so there’s less waiting for you and the patient.

Great Patient Education Tool

The beauty of digital is in the fact that you can enhance the image to bring out diagnostic detail.  You can magnify, heighten contrast, and even colorize the affected area.  It’s a great way for chiropractors to educate their patients about treatments and better demonstrate a misalignment or disk problem. For example, you can do a side-by-side comparison with a prior X-ray to show positive therapeutic changes. Your patients will actually be able to see, as well as feel, the physical improvement after treatment.

Dramatic Decrease in Need for Retakes

You have greater latitude in getting good readable images.  Digital is much more forgiving of exposure errors because it has a wider dynamic range than film.  If an image is under or over exposed, the computer can adjust for the error and provide a very useable image.  With film, an error in exposure often means that the X-ray must be repeated, which means that the patient must be irradiated a second time.  This is not only inconvenient, but results in unnecessary added radiation exposure. With digital, there are significantly fewer retakes. 

Is CR Right for Your Practice?

Computerized radiography offers the advantage of quick image access and does away with the need for stockpiling, searching and copying films.  All images are saved for easy retrieval on the computer system and stored on secured backups.

You can transmit digital images electronically in an instant to a colleague across town for consultation or diagnostic confirmation.  The image can be e-mailed while the patient is still in your office. If a patient wishes to have a copy of his or her X-rays, the images can simply be burned onto CD’s in a matter of minutes for just pennies. Simply hand the CD to your patient to take with him.

In addition, CR is a superior method of radiography because it’s faster; you can shave 10 to 15 minutes off a patient’s office visit.  Plus, digital images can be enhanced for greater clarity so that more diagnostic information can be derived from them.  Also, instead of manually drawing measurements directly on the film using a ruler and protractor, the computer can be programmed to automatically provide accurate measurements for you.

The use of computed radiography eliminates concerns about environmentally hazardous chemical waste disposal.  Across the country, government regulations continue to make disposal increasingly more costly and difficult.

Select the Right System and Service

If you do decide that your office could benefit from the advantages of computed radiography, make sure that you research not only the systems, but also their customer support.  As a new user of unfamiliar technology, the technical assistance, training and service a dealer and manufacturer can provide is critical.  While it’s easy to use, you and your staff will still need to learn how to adjust to and use the new equipment, and you’ll want to be able to quickly troubleshoot problems and get answers right away.  Make sure the manufacturer provides excellent customer service.
 
Conclusion

Many of today’s newer offices are fully computerized and are starting out paperless and filmless.  But practices with existing film radiography in place have to weigh the benefits of digital against its costs.  If you are doing a considerable amount of scans each day, then the advantages of switching are obvious; but for those practices that take less than five scans per day, the decision may be less focused on savings and more on getting faster, better results and maintaining a cleaner environment.  CR provides the practitioner with a paperless office where images are conveniently stored with each patient’s file on the computer hard drive and in backup systems.

Since 1985, Fred Fischer has been the senior executive at ALLPRO Imaging, a manufacturer of X-ray equipment for the medical profession. The company was founded in 1962.

Fred Fischer has been the senior executive at AllPro Imaging, Inc., a manufacturer of X-ray equipment for the medical profession, since it was established in 1985. A native of Hollywood, CA, Fred is a graduate of Manhattan College with a degree in electrical engineering. After his discharge from the service, Fred worked as an electrical engineer at RCA Corp., and was later a salesman for the Electrodyne Division of Becton Dickenson Corp.

For more information about ALLPRO and the ScanX 14, call Linda Schutt at 516-214-5611 or e-mail This e-mail address is being protected from spambots. You need JavaScript enabled to view it . Also, visit ALLPRO’s website at www.allproimaging.com.

Choosing the right laser for your light therapy can be extremely confusing, because the literature available on light therapy is not only confusing but contradictory.  Laser light has unique physical properties that no other light source or LED has. There is a big difference between a colorful brochure and the clinical efficacy of the unit being sold.  To date, laser instruments have been sold which do not even contain a laser. To help you make the right choice, this article defines the common terms used in light therapy and presents the biological basis of the unique clinical efficacy of Low Level LASER Therapy.

The word LASER is an acronym for Light Amplification by Stimulated Emission of Radiation.  Scientists recognize lasers by two parameters.  Laser light is coherent (single wavelength) and collimated (focused).  Coherent light means waves of the light quanta or photons are synchronous and move in the phase with each other.  By collimating or focusing a specific wavelength of light, energy can broadcast great distances and remain a focused dot of energy.  Advertised light therapy units, such as the LED, CO2, infrared or near-infrared lasers, are, in general, not collimated.  Removing the collimator from a laser will cause the light array to look just like an LED or any other colored light, but the biological and clinical effects are not the same. Laser light is the only source of coherent and collimated light.  This underlies the biological basis of light therapy.

While there is no legal definition for “Low-Level Laser Therapy (LLLT), most scientists and clinicians agree that Low-Level means that the power output is low enough not to raise the temperature of the tissue being irradiated by more than 1 degree.  The FDA classifies lasers with this power output as Class IIIa lasers.  Any potential danger from a Class IIIa laser results from direct irradiation of the eyes. Thermal damage is not possible. Class IIIa lasers allow LASERS to be used as therapeutic tools to, “… relieve pain and suffering and above all else, DO NO HARM….”

Low-level light therapy works by stimulating a cell’s innate metabolism.  Again, the effects are biochemical, not thermal and, therefore, cannot damage living cells.  The therapeutic effects of LLLT result from biomodulation of a tissue. Low-Level Laser Therapy is safe for both operator and patient.  LLLT lasers are therapeutic, because they allow living tissue to maintain or return to homeostasis without damaging tissue.

Four distinct biological effects occur when using LLLT, i.e., when photon energy is transferred to a biological chromophore.  These include:

1. Growth factor production occurs within cells and tissue in response to increased ATP and protein synthesis.

2. Pain relief results from suppression of the nociceptor response mediated by increased serotonin and endorphin release.

3. Immune-modulation and mitigation of the inflammatory response occur because the mononuclear phagocytic cells, mast cells, and leukocytes are stabilized, preventing the release of harmful inflammatory mediators. In addition, vasodilatation and increased microcirculation allows a rapid return to homeostasis and promotes first intention healing.

4. Direct trigger point stimulation allows direct release of endorphins and other endogenous pain mediators, such as serotonin, VIP, substance P, prostaglandins, etc.

Propagation of light though tissue is regulated by reflection, penetration, or absorption and transfer of energy of light quanta to the cell.  This is laser dependent.

Reflected energy becomes scatter radiation and is dangerous to both operator and patient.  This is a natural protection mechanism. The body could never control its internal environment, temperature, and, therefore, cellular metabolism, if all exposed photon energy was transferred to the tissue. The majority of energy from uncollimated and noncoherent light sources is reflected off the skin surface.  Most infrared light sources are uncollimated or noncoherent, or both, and depend on scatter or reflection to reduce the thermal damage due to irradiation.  Therefore, very little photon energy is transferred to the tissue.

As advertised, photon energy from high-power infrared lasers penetrates deep into the tissue.  Again, this is a physical and thermal phenomenon, not a therapeutic phenomenon.  Energy is dissipated as heat.  Thermal activation overrides the cells homeostatic metabolic state.  The cell may be turned on or off, but not in a functional manner. This can cause damage deep in tissues, out of sight of the clinician.  Furthermore, energy transfer to a biological chromophore does not occur.

When light quanta are absorbed, energy is transferred to water, some organic molecule, or to one or more chromophores within tissue, thereby producing a cellular response which changes the cell’s homeostatic set point.

Within the cell, the signal is transduced and amplified by a photon acceptor (chromophore).  When a chromophore first absorbs light, electronically excited states are stimulated, and primary molecular processes are initiated which lead to measurable biological effects.  These photobiological effects are mediated through a secondary biochemical reaction, photosignal transduction cascade, or intracellular signaling which amplifies the biological response.

The ionizing effects of LLLT allow photon acceptors to accept an electron. This turns on the oxidation-reduction cycle of the stimulated chromophores, such as Cytochrome oxidase, hemoglobin, melanin, and serotonin.  Changing the re-dox state of the chromophore changes the biological activity of that chromophore; e.g., hemoglobin changes its oxygen carrying capacity. This is in contrast to the destructive ionizing effects of X-rays, which remove or disrupt electrons from an atom or molecule and damage tissue.

When photon energy breaks a chemical bond, changes occur in the allosteric proteins in cell membranes (cell, mitochondrial, nuclear) and monovalent and divalent fluxes activate cell metabolism and intracellular enzymes directly.  Direct activation of cell membranes alters ion fluxes, particularly calcium, across that membrane.  Changes in intracellular calcium alter the concentrations of cyclic nucleotides, causing an increase in DNA, RNA, and protein synthesis, which stimulate mitosis and cellular proliferation.

When all of the above occur correctly, the photon activates a chromophore and that single enzyme molecule rapidly catalyzes thousands of other chemicals similar to the well known, calcium regulated, 2nd messenger cAMP cascade. This biological amplification process explains how low-power laser therapy can produce such profound systemic, cellular, and clinical effects.

One of the most confusing aspects of light therapy is dozens of published reports, which fail to find any effect from LLLT.  As with any treatment, clinical efficacy depends on diagnosis, dosage, treatment technique and individual reaction.  Similarly, each stage of the biomodulation cascade depends on additional laser specific factors, including the light source, wavelength, irradiation dose, power density, and tissue specific factors.  Alterations in any of these parameters can minimize or cancel the effects of light therapy. Here are some basic examples:
 
Light sources: A cell’s response to light differs markedly in vivo and in vitro.  The coherent properties of laser light are not important in cell suspensions or tissue culture monolayers.  In vitro, coherent or noncoherent light (both lasers and LED’s) with the same wavelength, intensity, and dose can stimulate the same biological response.  However, in vivo, in living tissue, only photons of coherent light are able to pass through optical windows in cell membranes to become accepted by photon acceptors (chromophores).

Coherent light is only created by a LASER light source, not from LED or SLD light sources.  Even coherent light, if left uncollimated, will, for the most part, reflect off the skin as dangerous scatter radiation. Coherent, collimated, laser light has, by far, the greatest therapeutic potential.  Because laser light triggers the cells own homeostatic mechanism, only low intensities and doses are required for dramatic biological responses.

Wavelengths: Every chromophore has an absorption coefficient for peak activation, which is wavelength specific. However, each chromophore has a wide range of wavelengths in which it will accept or donate electrons. Within living tissue, peak activation of a chromophore can occur within a broad range of wavelengths (e.g., oxygenated hemoglobin has absorption peaks at 420 and 577 nm; reduced hemoglobin at 560nm).  Wavelengths longer than 1200 nm (infrared) and shorter than 200 nm (ultraviolet) are absorbed by inter- and intracellular water.

Wavelengths of 620-720 nm are typi-cally better able to penetrate optical windows in cellular membranes because their photons are not easily absorbed by living tissue which, on average, are composed of 70-80% water. Chromophores found in eukaryotic (mammalian) tissue have peak activation spectra between 600 nm to 720 nm.   Since laser light acts as a trigger for normal cellular metabolism, it is not necessary to utilize a wavelength that strikes the peak activation of each chromophore.  It is only necessary for the wavelength to fall within the spectra of the chromophore.  The wavelength of 635 nm is contained within the spectra of the chromophores found in mammalian tissue and, therefore, has the potential to biomodulate all eukaryotic tissue.

Irradiation Dose: The product of power density (mW) and exposure time defines the irradiation dose and is measured in Jules of energy per square centimeter (J/cm2).  This is an extremely important parameter for laser treatment and biomodulation.  Scientists have shown the therapeutic efficacy of LLLT is enhanced by repetitive low doses within a specific time, in contrast to the same total dose in a single treatment. In addition, the biomodulation effects of LLLT are cumulative.  Repeated doses, within relatively short intervals, produce greater biological responses than single frequency lasers. Doses which are too low produce no effect.  Doses which are too high produce no effect or dampen biological activity.  Each biological tissue has an optimal dose, which is laser dependent.

Power density from 2 to 5 mW is adequate to activate mammalian chromophores. Power higher than 5 mW may exceed the activation levels of some chromophores. The greatest biomodulation is created with repeated doses of pulsed collimated laser light at or around 5 mW of power.

Chromophore response is dependent upon the functional metabolic state and composition of the tissue at the time of irradiation. LLLT produces separate responses in separate tissue based on the active chromophore within that tissue, e.g. bronchial tissue (mast cells), skin (melanin).  Healthy, injured, and malignant tissues absorb light, or transfer energy differently, because they contain different chromophores, and are in different metabolic states.  This explains the wide array of therapeutic effects of the LLLT in damaged tissue and the lack of response in healthy tissue.

The most dramatic examples include the different effects of LLLT irradiation on healthy tissue, inflamed tissue, and malignant tissue. Healthy tissue does not contain a high concentration of biologically active chromophores (e.g., biogenic amine, histamine, serotonin, VIP, substance P), while inflamed tissue does. LLLT can mitigate the inflammatory response by stabilizing mononuclear phagocytic cells, stimulating leukocyte chemotaxsis, and preventing mast cell degranulation.  This prevents the release of histamine, and other biogenic amines, which cause the cellular infiltration responsible for the four cardinal signs of inflammation: redness, heat, pain, and swelling.  LLLT dampens the inflammatory cascade, mitigates inflammation, and allows first intention healing.  Similarly, malignant tissue is defined by its high mitotic index, which supports the rapid, uncontrolled growth of cancer.  Mitotic cells appear insensitive to LLLT irradiation while injured and dormant cells can be stimulated to divide.

While LLLT may have no effect on a healthy, normal cell, it has profound biological and therapeutic effects on inactive, sick or injured cells.  The power of LLLT lies in the fact that injured cells respond to irradiation, turning on or off, allowing the cell to return to, or maintain, cellular homeostasis.  In short, LLLT allows the cell to heal itself.
 
In conclusion, for safe and effective light therapy, the ideal therapy device should be a low powered (between 2 and 5 mW), laser (capable of producing collimated and coherent light), which produces wavelength between 600 than 720 nm, and is capable of rapidly delivering pulsed frequencies to tissue.

R. Gerry Graham, DC, is a licensed chiropractor, graduate of Logan College of Chiropractic and practices in Aurora, Colorado. Dr. Graham is President of LED Healing Light LLC.

Joan M. Murnane holds a PhD from Emory University School of Medicine, a DVM from the College of Veterinary Medicine, University of Georgia and a Masters in Pharmacology and Physiology from Washington State University College of Veterinary Medicine, Pullman, Washington.

For additional information or dates for upcoming seminars, please email This e-mail address is being protected from spambots. You need JavaScript enabled to view it .