| Allicdata Part #: | 1531830000-ND |
| Manufacturer Part#: |
1531830000 |
| Price: | $ 35.13 |
| Product Category: | Uncategorized |
| Manufacturer: | Weidmuller |
| Short Description: | UR20-PK-1510690000-SP |
| More Detail: | N/A |
| DataSheet: | 1531830000 Datasheet/PDF |
| Quantity: | 1000 |
| 1 +: | $ 31.93470 |
| Series: | * |
| Part Status: | Active |
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Applied Nuclear Magnetic Resonance (NMR) spectroscopy is a technique employed in numerous scientific and industrial fields, including medicine, chemical engineering, physics, materials science, and biophysics. Its primary purpose is to measure small magnetic fields, such as those produced by the nucleus of an atom, so that their properties can be studied. In the past, application of nuclei magnetic resonance (NMR) was quite limited; however, advancements in technology, such as portable NMR instruments, are increasingly making this technology accessible and leading it to greater application fields. Understanding the workings of an NMR system and its major components, including receiver coils, rfplatters and probes, magnetic fields, and various software tools, are key to being able to take full advantage of this powerful technology.
The basic working principle of a nuclear magnetic resonance (NMR) system is relatively straightforward. A powerful external magnetic field is applied to the sample, which causes some atoms of the sample to have nuclear spins that are aligned along the magnetic field. When a radio frequency (RF) pulse is sent through the sample, the aligned spins of the exciting nuclei are affected differently, depending on the nucleus. Those nuclei that are magnetized in the same direction as the external magnetic field experience no change due to the RF pulse. However, those nuclei that are magnetized in the opposite direction to the external magnetic field are affected by the RF pulse, which causes their spin axis to rotate. As the nuclei return to their original positions, they emit energy, which can be measured by receiver coils and used to construct a spectrum.
The receiver coils of a nuclear magnetic resonance (NMR) system are used to detect the NMR signals. The NMR signals are received in two orthogonal receiver coils, known as the FID, or free induction decays, which measure the phase and magnitude of the NMR signal. The signal is then amplified by a low noise amplifier, which filters out any other signals that may be present. The filtered signals are then digitized and passed on to further software processing, which converts the signals into a raw FID spectrum.
NMR probeheads form a vital part of the NMR system. There are several types of probes available, including fixed and variable probes. Fixed probes are used for measurements on a limited range of samples, and variable probes are used for measurements on a wider range of samples. The probe heads contain the rf coil used to transmit the RF pulse to the sample, as well as the two receiver coils used to detect the NMR signals from the sample. The probe heads also contain a precision high-frequency amplifier, which amplifies the NMR signal before it is digitized and passed on to further processing.
The application of NMR spectroscopy has widened significantly in recent years, with advances in the technology making it possible to use portable NMR instruments. NMR is an essential tool in many fields, including biology, chemistry, material science, and medicine. It is used to study a wide range of chemical, physical, and biochemical systems, from drug delivery systems to the structure of DNA. In addition, NMR can be used to study the properties of proteins, helping researchers to design effective drugs. It can also be used to monitor reactions in real-time, allowing for the optimization of production processes and the design of more efficient and eco-friendly processes.
Nuclear magnetic resonance (NMR) spectroscopy is a powerful technology with a wide range of applications. The basic working principle is relatively simple, and involves the application of a powerful external magnetic field to the sample, with a resulting emission of energy when the nuclei return to their original spin positions. The signal is detected by receiver coils and amplified by a low noise amplifier, before being digitized and further processed. NMR probes are also an important component of the system, which come in various types depending on the range of samples to be measured. Advances in technology have made it increasingly possible to use portable NMR instruments, bringing NMR spectroscopy to a wider range of applications.
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|---|
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| 7-1531047-7 | TE Connectiv... | 302.48 $ | 1000 | FA HD-I SPARE PART KIT |
| 1531110000 | Weidmuller | 8.25 $ | 1000 | BL 3.50/13/180LR SN OR BX |
| 1531099-1 | TE Connectiv... | 2.08 $ | 1000 | FA HD-I EMPO..110F.150OV ... |
| HFBR-1531ETZ | Broadcom Lim... | -- | 9690 | TX OPT HIGH PERFORMANCE 5... |
| 1531330000 | Weidmuller | 6.99 $ | 1000 | BLZF 3.50/11/180LR SN OR ... |
| 1531200000 | Weidmuller | 16.58 $ | 1000 | BL-I/O 3.50/10LR NPN LED ... |
| 1531031-1 | TE Connectiv... | 2.77 $ | 1000 | FA HD-I EMPO080F100OVL BE... |
| 1531 | Greenlee Com... | 0.0 $ | 1000 | TOOL TESTER PATCH-CHECK P... |
| 1531866 | Phoenix Cont... | 0.0 $ | 1000 | CABLE 3POSCable Assembly |
| 1531882 | Phoenix Cont... | 0.0 $ | 1000 | CABLE 3POSCable Assembly |
| 1531250000 | Weidmuller | 3.53 $ | 1000 | BLZF 3.50/05/180LR SN OR ... |
| 153108 | TE Connectiv... | 0.0 $ | 1000 | CONN RING CIRC 16-18AWG #... |
| 1531000000 | Weidmuller | 2.11 $ | 1000 | BL 3.50/03/180LR SN OR BX |
| 1531100000 | Weidmuller | 7.63 $ | 1000 | BL 3.50/12/180LR SN OR BX |
| 15315 | Wiha | 4.82 $ | 1000 | SCREWDRIVER PHILLIPS #1 1... |
| 1531130000 | Weidmuller | 9.0 $ | 1000 | BL 3.50/15/180LR SN OR BX |
| 1531037-1 | TE Connectiv... | 2.77 $ | 1000 | FA HD-I EMPO120F155OV BEN... |
| 1531921 | Phoenix Cont... | 0.0 $ | 1000 | CABLE 4POSCable Assembly |
| 70152-1531 | Omron Automa... | 208.01 $ | 1000 | SAFETY EDGE |
| 1531027-1 | TE Connectiv... | 2.08 $ | 1000 | FA HD-I EMPO120F170F BENC... |
| 1531093-1 | TE Connectiv... | 2.08 $ | 1000 | HD INDL NON-AMP APPLITool |
| 75-153123130659 | City Technol... | 385.86 $ | 10 | MINI O3 3E 1 F TRANSMITTE... |
| 1531A2L12 | APEM Inc. | -- | 1000 | SWITCH TOGGLE SPST 10A 12... |
| 1531035-1 | TE Connectiv... | 2.08 $ | 1000 | HD INDL NON-AMP APPLITool |
| 1531051-1 | TE Connectiv... | 2.08 $ | 1000 | HD INDL NON-AMP APPLITool |
| 44505-1531 | Omron Automa... | 68.73 $ | 1000 | SL-AL21MM PLAST 2N/C+1N/O... |
| 15313 | Keystone Ele... | 16.51 $ | 1000 | BOARD TERM TURRET DBL 19P... |
| 15310 | Keystone Ele... | 25.51 $ | 1000 | BOARD TERM TURRET DBL 33P... |
| 1531106-1 | TE Connectiv... | 2.08 $ | 1000 | HDI/FA E/MPO.070F.090O/LM... |
| 1531370000 | Weidmuller | 9.0 $ | 1000 | BLZF 3.50/15/180LR SN OR ... |
| 1531110-1 | TE Connectiv... | 2.08 $ | 1000 | HDI/FA E/M./LM/G/CUTTool |
| 1531044-1 | TE Connectiv... | 3.47 $ | 1000 | FA HD-I EMPO080F120F LM/ ... |
| 1531963 | Phoenix Cont... | 0.0 $ | 1000 | CABLE 5POSCable Assembly |
| 1531060-1 | TE Connectiv... | 2.08 $ | 1000 | HD INDL NON-AMP APPLITool |
| D4C-1531 | Omron Automa... | 72.58 $ | 1000 | LIMIT SW SEAL PIN PLUNGER |
| 1531824 | Phoenix Cont... | 0.0 $ | 1000 | CBL 5POS 7/8" 16UNF PLUG-... |
| 7-1531025-7 | TE Connectiv... | 337.79 $ | 1000 | FA HD-I SPARE PART KIT |
| 153117 | FLIR | 22.17 $ | 1000 | AC ADAPTER, 117VAC |
| 1531140000 | Weidmuller | 9.6 $ | 1000 | BL 3.50/16/180LR SN OR BX |
DIODE GENERAL PURPOSE TO220
CB 6C 6#16 SKT RECP
CA08COME36-3PB-44
CA-BAYONET
CB 6C 6#16S SKT PLUG
CAC 3C 3#16S SKT RECP LINE
1531830000 Datasheet/PDF