NEW CUSTOM-CAL CC50-3.5-26 SALES and CUSTOM-CAL CC50-3.5-26 CALIBRATION

 
Custom-Cal has for sale a new CUSTOM-CAL CC50-3.5-26. Also, short calibration turn times minimize downtime and reasonable rates decrease your long-term cost of ownership and minimizes downtime of the CUSTOM-CAL CC50-3.5-26. We specialize in quick turnaround times and we can handle expedited deliveries upon request.

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List Price for a new CUSTOM-CAL CC50-3.5-26, $3,850.00   CUSTOM-CAL CC50-3.5-26   Description / Specification:    
CUSTOM-CAL CC50-3.5-26 50 ohm 26.5 GHz 3.5 mm Calibration Kit

The Custom-Cal CC50-3.5-26 is a 50 Ohm, DC to 26.5 GHz, 3.5 mm-type Standard Calibration Kit. It consists of a; CC-5002-OF Open Female Connector, CC-5002-OM Open Male Connector, CC-5002-SF Short Female Connector, CC-5002-SM Short Male Connector, CC-5002-LF Load Female Connector, CC-5002-LM Load Male Connector, CC-5002-TF Through Female to Female Connector, CC-5002-TFM Through Female to Male Connector, CC-5002-TM Through Male to Male Connector, 7mm flat wrench and a 8710-1765CC 8 in-lbs [0.9 N.m] Break-Over Torque Wrench..
Specifications.
Open Female Connector.
Frequency Range: DC to 26.5 GHz.
Impedance: 50 Ω.
Phase (DC to 3 GHz): 0.65 degree.
Phase (3 to 8 GHz): 1.2 degree.
Phase (8 to 26.5 GHz): 2 degree.
Open Male Connector.
Frequency Range: DC to 26.5 GHz.
Impedance: 50 Ω.
Phase (DC to 3 GHz): 0.65 degree.
Phase (3 to 8 GHz): 1.2 degree.
Phase (8 to 26.5 GHz): 2 degree.
Short Female Connector.
Frequency Range: DC to 26.5 GHz.
Impedance: 50 Ω.
Phase (DC to 3 GHz): 0.65 degree.
Phase (3 to 8 GHz): 1.2 degree.
Phase (8 to 26.5 GHz): 2 degree.
Short Male Connector.
Frequency Range: DC to 26.5 GHz.
Impedance: 50 Ω.
Phase (DC to 3 GHz): 0.65 degree.
Phase (3 to 8 GHz): 1.2 degree.
Phase (8 to 26.5 GHz): 2 degree.
Load Female Connector.
Frequency Range: DC to 26.5 GHz.
Impedance: 50 Ω.
Return Loss (DC to 3 GHz): 44 dB minimum.
Return Loss (3 to 6 GHz): 36 dB minimum.
Return Loss (6 to 26.5 GHz): 30 dB minimum.
Load Male Connector.
Frequency Range: DC to 26.5 GHz.
Impedance: 50 Ω.
Return Loss (DC to 3 GHz): 44 dB minimum.
Return Loss (3 to 6 GHz): 36 dB minimum.
Return Loss (6 to 26.5 GHz): 30 dB minimum.
Through Female to Female Connector.
Frequency Range: DC to 26.5 GHz.
Impedance: 50 Ω.
Insertion Loss (DC to 26.5 GHz): 0.2 dB maximum.
Return Loss (DC to 8 GHz): 30 dB minimum.
Return Loss (8 to 18 GHz): 28 dB minimum.
Return Loss (18 to 26.5 GHz): 26 dB minimum.
Through Female to Male Connector.
Frequency Range: DC to 26.5 GHz.
Impedance: 50 Ω.
Insertion Loss (DC to 26.5 GHz): 0.2 dB maximum.
Return Loss (DC to 8 GHz): 30 dB minimum.
Return Loss (8 to 18 GHz): 28 dB minimum.
Return Loss (18 to 26.5 GHz): 26 dB minimum.
Through Male to Male Connector.
Frequency Range: DC to 26.5 GHz.
Impedance: 50 Ω.
Insertion Loss (DC to 26.5 GHz): 0.2 dB maximum.
Return Loss (DC to 8 GHz): 30 dB minimum.
Return Loss (8 to 18 GHz): 28 dB minimum.
Return Loss (18 to 26.5 GHz): 26 dB minimum.



 

Standard Calibration $510.00 *
*This is a Web introductory price for one calibration of the CUSTOM-CAL CC50-3.5-26. Price does not in most cases include measurement performance data. Pricing does include NIST traceable calibration and issue of a calibration certificate and calibration label. Pricing may vary slightly due to volume and location of laboratory supporting calibration. Volume pricing may apply. On-site fees may apply depending on logistics, location and volume of work to be completed during the visit.


Related RF Terms and Definitions. For a complete list go to our  Terms and Definitions Page.

Available Gain
Available Gain is the ratio, at a specific frequency, of power available from the output to the power in from the source.

Frequency Span
Frequency Span specifies the range between the start and stop frequencies, also referred to as bandwidth

Peak Envelope Power
Peak envelope power is the maximum value of the envelope power. Envelope power is measured by making the averaging time much less than 1/fm where fm is the maximum frequency component of the modulation waveform. The averaging time is therefore limited on both ends: (1) it must be small compared to the period of the highest modulation frequency, and (2) it must be large enough to be many RF cycles long.


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