datasheet,schematic,electronic components, service manual,repairs,tv,monitor,service menu,pcb design
Schematics 4 Free
Service manuals, schematics, documentation, programs, electronics, hobby ....


registersend pass
Bulgarian - schematics repairs service manuals SearchBrowseUploadWanted

Now downloading free:Stanford Research Systems www.thinksrs.com-phase

Stanford Research Systems www.thinksrs.com-phase free download

Various electronics service manuals

File information:
File name:www.thinksrs.com-phase.pdf
[preview www.thinksrs.com-phase]
Size:174 kB
Extension:pdf
Mfg:Stanford Research Systems
Model:www.thinksrs.com-phase 🔎
Original:www.thinksrs.com-phase 🔎
Descr: Stanford Research Systems www.thinksrs.com-phase.pdf
Group:Electronics > Other
Uploaded:14-12-2019
User:Anonymous
Multipart:No multipart

Information about the files in archive:
Decompress result:OK
Extracted files:1
File name www.thinksrs.com-phase.pdf

Introduction: This application note Spectral Density of Phase Fluctuations discusses various techniques for the S(f) measurement of phase noise using frequency domain analysis. Typical This is the most basic measure of phase applications areas are characterization of noise. It is the square of the Fourier phase noise in crystal oscillators, phase transform of the time varying phase (t) noise of synthesized sources and phase normalized to a 1 Hz bandwidth. The noise in PLL or other measurement spectrum is normalized because when systems. These methods should give measuring a broadband signal such as good estimates of phase noise for noise, the amplitude of the spectrum frequencies upto 2 GHz. Frequency changes with the bandwidth over which stability in the microwave region is not the measurement is made. Normalizing covered. allows measurements with different bandwidths to be compared. If the noise Concepts of frequency stability: is Gaussian in nature, the amount of noise in other bandwidths may be Instantaneous frequency can be defined approximated by scaling the spectral as the time rate of change of phase, i.e. density by the bandwidth. Using the d(t ) above example of phase modulation, 2 (t ) ( t ) dt S(f) can be written as where (t) is the instantaneous phase of 2 rms ( f ) S ( f ) = the oscillator, and the angular frequency B is where rms = / 2 and B is the 2f . bandwidth (in Hz) used to measure The instantaneous output voltage of a rms. S(f) describes the phase noise at DUT may be written as an offset f on both sides of the carrier. V ( t ) = [Vo + (t )] sin[2v o t + (t )] where Vo and vo are the nominal Single Sideband Phase Noise L(f) amplitude and frequency of the output, and it is assumed that This is the most common way to express (t ) a phase noise spectrum. L(f) is defined << 1 and as the ratio of power in a single 1 Hz Vo sideband at an offset frequency f to the . (t ) total signal power. Typically, when << 1 measuring phase noise, almost all of a 2v o t signal's power is in the carrier, so carrier for s

>> View document online <<



>> Download document << eServiceInfo Context Help



Was this file useful ? Share Your thoughts with the other users.

User ratings and reviews for this file:

DateUserRatingComment

Average rating for this file: 0.00 ( from 0 votes)


Similar Service Manuals :
Stanford Research Systems www.thinksrs.com-SIM928c - Stanford Research Systems www.thinksrs.com-SG384 CarrierSuppress IQ - Stanford Research Systems www.thinksrs.com-SG300 comparison - Stanford Research Systems www.thinksrs.com-SC10c - Stanford Research Systems www.thinksrs.com-RightQuad - Stanford Research Systems www.thinksrs.com-RGAm - Stanford Research Systems www.thinksrs.com-RGAc -
 FB -  Links -  Info / Contacts -  Forum -   Last SM download : Aiwa CT-X105

script execution: 0.02 s