Product Details:
| Minimum Order Quantity | 1 Piece |
| Material | Steel |
Additional Information:
Product Details:
| Application Area | For Oven/ Furnace |
| Control Type | PID |
| No of digits | 4+7 |
| Display Size | 48*48 mm |
| Output type | SSR |
| Mounting Type | Surface Mounting |
| Sensor Input | Thermocouple |
| Voltage | 220-240 V |
Product Details:
| Material | screen printer |
| Object To Be Printed | laboratory |
| Usage/Application | Laboratory |
| Power | CUSTOMIZED |
| Automation Grade | Semi Automatic |
Product Details:
| Voltage | 230 V |
| Categories | Diagnostic Equipments |
Interferometer is built by assembling the building blocks on a breadboard as per desired optical layout. Optics and laser head are held using kinematic mounts with two axis fine adjustment facility. Precision alignments for obtaining the interference fringes are done using kinematic mounts.
One of the simplest experiments using the interferometer is measurement of index of refraction of air with an airtight test cell placed in one of the optical arms of the interferometer. No other factor such as convective airflow, should be present, that can generate optical path differences. The flexibility in fringe localization is one of the important advantages of the mach zehnder interferometer over other interferometers. Although many Mach-Zehnder interferometers use a rectangular arrangement, parallelogram arrangements are also possible. Vibration isolated supports for optical table is optional.
Product Details:
| Minimum Order Quantity | 1 Kg |
| Brand | Dycotec |
| Form | paste |
| Packaging Size | 100 grams |
| Ph Value | N/A |
| Usage | biomedical sensors, automotive, electrodes, aerospace, printed heaters, printed resistors, membrane |
Additional Information:
Product Details:
| Voltage | 230 V |
| Categories | Examination Equipments |
Fizeau Interferometer is one of the simplest and most versatile interferometers and is popular for routine measurements of both flat and spherical surfaces. It is used to measure optical components such as flats, prisms, lenses, or precision metal parts such as bearings, sealing surfaces or polished ceramics. Measurements can be made by using the static fringe analysis software.
The Holmarc Fizeau interferometer (model no:HO-ED-INT-14) basically comes with high optical quality (λ / 20) reference flat. The reflection from the test surface interferes with the reflection from reference flat, producing fringes. The shape and quality of the fringes depends on surface quality of the test flat. The fringes are digitalized using a high resolution CCD camera. By analyzing the fringes, we can obtain the P-V flatness, RMS flatness, 3D surface plot etc. The instrument is built upright to fix the test sample easily. The tip / tilt test base allows the test sample to align with the reference surface. High quality aberration corrected optical design enhances performance.
Holmarc's Brewster's Angle Apparatus (Model No: HO-ED-P-01) is designed to study the Brewster’s angle phenomenon and the polarization of reflected light. The essential elements of the apparatus consists of a goniometer, a laser light source capable of projecting a light beam that is linearly polarized in its plane of incidence, and a pinhole photo detector with output measurement unit for detecting and measuring the intensity of light reflected. The diode laser and polarizer rotator are mounted on an optical rail.
Intensities of reflected light polarized in the plane of incidence and perpendicular to the plane are obtained as a function of angle of incidence. The results should be consistent with Fresnel's laws of reflection.
A beam of light incident on a di-electric transparent material can be resolved into parallel (P) and orthogonal (S) components. These components have different reflection coefficients and Brewster discovered that at a particular angle of incidence Ɵв (called Brewster angle), reflection co-efficient of P-component goes zero. At this angle, direction of reflected and transmitted beam are orthogonal to each other.
Product Details:
| Minimum Order Quantity | 1 Set |
| Capacity(Kg) | 100 kg |
| Material Loading Capacity | Customer Specification |
| Power Source | Customer Specification |
| Usage/Application | Customer Specification |
| Melting Material | Customer Specification |
| Max Temperature | 1000-1500 degree Celsius |
| Power | Customer Specification |
| Country of Origin | Made in India |
Additional Information:
Product Details:
| Stage | Two Stage |
| Material | Stainless Steel |
| Flow Rate | 50 m3 |
| Type | Belt Drive Rotary Vane Pumps |
Product Details:
| Minimum Order Quantity | 1 Piece |
| Capacity(Kg) | 100 kg |
| Material Loading Capacity | 0-500 kg |
| Max Temperature | 1000-1500 degree Celsius |
Additional Information:
Product Details:
| Brand | Spectro |
This device is specifically designed for studying reflection gratings. It consists of a laser head mounted on a kinematic holder and a grating mount with angular adjustments. The grating can be fixed at appropriate angles using this mount. Fine adjustments in grazing or incident angle can be done using kinematic tuning of the laser mount.
Both the laser and grating mounts are fixed on rail carriers, which are held on a graduated solid aluminum rail. The diffraction pattern is projected on a screen or wall. When a meter scale is used as reflection grating, the pattern can be observed typically at two to three meters.
More +
Experiment
To measure the wavelength of laser light using a millimeter scale as gratingProduct Details:
| Usage/Application | Laboratory Analysis |
| Automation Grade | Automatic |
Product Details:
| Brand | Spectro |
2. Precise travel adjustment provided for CMOS with Optics assembly to fine focus the image.
3. Manual dispensing.
4. 50, 100 & 250 micro liter sample syringes provided with the system.
5. Precision height adjustment provided at the test base.
6. Vibration inhibiting solid construction for sharp drop images.
7. Powerful and user friendly windows software provided for image analysis.
8. Live images can be viewed on the PC monitor showing the droplet on the solid surface reassures the operator-regarding validity of the contact angle measurement.
9. Video processing enabled software.
10. Captured image and its Angle measurement table can be saved for future reference.
Product Details:
| Voltage | 230 V |
| Categories | Diagnostic Equipments |
Computer interfaced Fabry-Perot interferometer (Model No:HO-ED-INT-10A) is similar to projection type (model no:HO-ED-INT-10), apart from the fact that in this case, the interference pattern is captured by a CCD sensor and displayed on a computer monitor. The advantage of computer interface is that the pattern can be saved for future analysis. In addition, measurements can be taken directly from the monitor by using the software module provided.
In the etalon, distance between partially reflecting mirrors can be precisely varied in microns. One of the beam splitters can be kinematically adjusted for initial settings
Product Details:
| Power | 3 kW |
| Categories | Diagnostic Equipments |
Holmarc's Young's modulus apparatus (Model No: HO-ED-M-02) is used to measure the Young's modulus of a bar. Young's modulus is a measure of stiffness of an elastic material and is a quantity used to characterize materials. It can vary considerably depending on the exact composition of the material. If the beam is loaded at its mid-point, the depression produced will not form an arc of a circle. This type of bending is called non-uniform bending. If the beam is loaded at both ends, the elevation produced will form an arc of a circle. This type of bending is called uniform bending. Two methods are used to measure Young's modulus of the bar in both uniform and non-uniform bending. They are Pin and Microscope method and Optic lever method.
More +A refractometer device used for the measuring the refractive index of samples using the concepts of critical angle and total internal reflection. Holmarc's Refractometer (Model No: HO-ED-O-03) is an experimental model designed for understanding the basics of refractometry.
More +
Experiment
To find the refractive index of an unknown solution.
Refractive index measurement is easy
Compact and precision design
High performance LED light source of optical wavelength 589nm
Precise optics minimize aberrations
Can observe clear and sharp shadow line
Mounts and rail with black anodized finish
The Z-Scan technique is a simple and popular experimental technique used to measure intensity dependent nonlinear susceptibilities of materials. Holmarc's Z-Scan System is a simple implementation of the z-scan technique that can be used to characterize optical materials.
In this method, the sample is translated along the axis of a focused Gaussian beam, and the far field intensity is measured as a function of the sample position. Analysis of the intensity versus sample position, Z-Scan curve, predicated on a local response, gives the real and imaginary parts of the third order susceptibility. In this technique, the optical effects can be measured by translating a sample in and out of the focal region of an incident laser beam
Holmarc's Photo Electric Apparatus (Model No: HO-ED-EM-02) is an instrument for studying the Photo Electric Effect and to obtain the Planck's constant.
A halogen source provides light energy to the photo tube. A filter wheel is placed in between the light source and photo tube to select different wavelengths. The filter wheel includes five narrow band interference filters to get the precise wavelength. A vacuum photo tube is kept inside the tube housing. This tube has very low anode dark current to achieve better results. The microprocessor controlled electronic interface gives the current and voltage readouts. The regulated power supply has 0 - 2V variable voltage to provide the stopping potential for electrodes. The ammeter gives accurate current output measurement facility. Toggle switch is provided to change the current range. The lamp house, filter wheel and photo tube housing are placed on an optical rail.Photo electric effect is the liberation of electrons from the surface of a material by absorption of energy from incident light. For each metal, there exists a minimum binding energy for electron, which is a characteristic of the element, called the work function. When a photon strikes a bound electron, it transfers its energy to the electron. If this energy is less than the metal's work function, the photon is remitted and no electrons are liberated. If this energy is greater than an electron's binding energy, the electron escapes from the metal with a kinetic energy equal to the difference between the photon's original energy and the electron's binding energy.
The stopping potential is measured by varying the anode voltage until the current drops to zero. The slope of a plot of stopping potential versus frequency is the value of the ratio, h/e. Hence the value of Planck's constant (h) and work function of the material can be determined. This instrument also imparts students, fundamental understanding of the quantum nature of light.
| Power supply | 230V AC, 50 Hz |
| Power cord | 3 core 3 pin |
| Operating voltage | 0 - 2 KV |
| Video system | High performance CCD sensor |
| Camera lens magnification | 30 X |
| Lighting | High bright LED lighting mechanism |
| Optical power | 1 W |
| Dimension | 590 x 490 x 760 mm |
Product Details:
| Capacity | 500 Litre |
| Automation Grade | Automatic |
| Display Type | Digital |
| Number Of Trays | 6 |
| Country of Origin | Made in India |
Product Details:
| Wavelength Range | 185-900 nm |
| Optical System | Single Beam |
| Mobility | Benchtop |
| Lamp Type | Xenon Lamp |
| Brand | Holmarc |
| Country of Origin | Made in India |
Confocal Raman spectroscopy is a powerful analytical technique that combines Raman spectroscopy with confocal microscopy. It allows spatially resolved chemical analysis of samples by providing high-resolution Raman spectra from specific locations within a sample. A focused laser beam is used to illuminate the sample using the microscope, and the Raman-scattered light is collected through the same objective lens and coupled to the spectrometer.
Holmarc CRM 216C is a fully automatic inverted infinity confocal microscope integrated with a high-resolution spectrometer and laser excitation system. The new ergonomic design helps the user capture the microscopic image and Raman spectrum easily. The color-corrected infinity design microscope has a motorized turret, filter wheel, switching mirror, sample stage, and focusing features. The turret comes with six slots for holding six different magnification microscope objectives. It is also equipped with an 8-slot automatic filter wheel for dielectric beamsplitters and a notch/edge filter combination for Raman and photoluminescence applications with different wavelength lasers. The viewing head is a stereo binocular head with a 5.0 MP CMOS camera, which gives clear, sharp, high-resolution images of the sample. The coaxial illumination and bottom LED illumination can be controlled by software. The hand-held controller provided with the system makes easy adjustments of the sample stage and LED control by using the joystick key.
Photoluminescence is one of the best scientific inventions ever in the field of material Science. The luminous efficiency of each fluorescent material differentiates them. And this experiment provides you the ratio of emitted photons to absorbed photons which is called the quantum yield of the material.
Our HO-SP-SQR300FA is our spectra monochromator with PMT detector which can be used as a PL system, which makes use of photoluminescence to measure the quantum yield of a material quickly and accurately. Our system consists of an excitation source, a monochromator and a photomultiplier tube as the spectrometer detector. It has a Czerny-turner optical path configuration; a plane holographic grating is used to diffract the input light. Use of holographic grating minimize the stray light for high sensitivity and accuracy. A stepper motor-controlled sine drive positions the grating, which is mounted on a precision rotary table. The sine drive delivers a linear relationship between stepper motor motion and wave- length of interest. Also, it includes a mechanism to change the wavelength selected by software and to record the resulting changes as a function of wavelength.
Holmarc has introduced new experiments for solar physics. It is a branch of astrophysics that specializes in exploiting and explaining the detailed measurements that are possible only for our closest star.
MoreXenon Arc lamps are excellent sources of continuous light. The bright emission from short arc between the anode and cathode makes these lamps high intensity point sources, capable of being collimated with the proper lens configuration or re imaged onto a fiber bundle.
In both models xenon arc lamp housing utilizes heat conductive forced air cooling technique, to make sure efficient cooling of the lamp and electronics. Lamp housing include condensing optics to produce a 25mm collimated light beam. 50mm collimated light beam can also be provided upon request.
Due to nonlinear atomic polarization, crystals can emit a different frequency of light other than absorbed. In order to see the second order effect of atomic polarization, which causes doubling in frequency of the incident light, the incident light must be intense and coherent source, like a laser. Potassium Dihydrogen Phosphate (KDP), Urea etc. are the crystals that exhibit nonlinear polarization properties. When light hits a crystal, it excites the atomic dipoles. In classical optics, it is assumed that this polarization of atoms is linear to the magnitude of electrical field of the incident light. In reality, this polarization is a nonlinear phenomenon, but the nonlinear components are evident only for high intensity.
The RHANDY is a very user friendly and economical solution for those requiring a portable radiation and contamination monitor. This portable handheld instrument will instantly detect and measure radioactivity on clothing, food, water and the environment.
The user selectable alarm thresholds can be set to the desired radiation levels or the recommended factory default alarm thresholds can be used. Operation of the RHANDY is completely automatic, once the easy-to-set operational parameters have been configured. Simply position the unit in close proximity to the object that needs to be scanned and listen for the varying audio alarm to sound and observe the large easy to read display.
In addition to the quick response, the RHANDY can be used to monitor accumulated dose. Locate the unit near the air intake of a building for the tracking of accumulated dose of air filters or intake pathways. Tracking of an air intake filter will provide vital information in determining when to shut down a system or when to change the filter
The RC22 and RC23 are designed to allow fast and easy inspection of areas, containers or vehicles that may contain radioactive material.
Fully automatic, the unit will set an alarm threshold after performing a background check. When radiation is detected, the display will immediately show the increasing radiation levels. An audio alarm will also be activated to help locate the exact source of the radiation. The tone varies based upon the proximity and intensity of the radioactive source.
The MSPEC is a fast responding palm size Spectroscopic Personal Radiation Detector (SPRD) that will instantly measure any material for the presence of radioactivity.
The MSPEC Gamma-Ray Spectrometer utilizes a Sodium doped Cesium Iodide crystal and state of the art electronics for the most accurate results.
Operation of the MSPEC is completely automatic, once the easy-to-set operational parameters have been decided. The system allows for displaying units of measure as Counts per Second (CPS), Dose-Rate (nSv/h), Exposure Rate (µR/h), or Accumulated Dose (nSv).
The MSPEC meets ANSI 42.48:2008 American National Standard Performance Requirements for Spectroscopic Personal Radiation Detectors (SPRDs) for Homeland Security.
Product Details:
| Laser Type | CO2 |
| Laser Power | 100 W |
| Usage/Application | Metal Engravers |
| Compatible Software | Auto CAD |
| Cooling Mode | Industrial Chiller |
| Operation Mode | Automatic |