Home
        Model 425A Delay Operating and Service Manual
         Contents
1.       Printed in U S A     Model 425A  Delay  Operating and Service Manual    ORTEC   Part No  733190  Manual Revision F    1202                Advanced Measurement Technology  Inc   a k a  ORTEC    a subsidiary of AMETEK    Inc     WARRANTY    ORTEC  warrants that the items will be delivered free from defects in material or workmanship  ORTEC makes no  other warranties  express or implied  and specifically NO WARRANTY OF MERCHANTABILITY OR FITNESS  FOR A PARTICULAR PURPOSE     ORTEC   s exclusive liability is limited to repairing or replacing at ORTEC   s option  items found by ORTEC to be  defective in workmanship or materials within one year from the date of delivery  ORTEC   s liability on any claim of  any kind  including negligence  loss  or damages arising out of  connected with  or from the performance or breach  thereof  or from the manufacture  sale  delivery  resale  repair  or use of any item or services covered by this  agreement or purchase order  shall in no case exceed the price allocable to the item or service furnished or any part  thereof that gives rise to the claim  In the event ORTEC fails to manufacture or deliver items called for in this  agreement or purchase order  ORTEC   s exclusive liability and buyer   s exclusive remedy shall be release of the  buyer from the obligation to pay the purchase price  In no event shall ORTEC be liable for special or consequential  damages     Quality Control  Before being approved for shipment  each ORTEC instrument 
2.  commonly used for  pulse work  skin effect losses in the conductor are  the predominant losses for frequency components  below approximately 1000 MHz  Skin effect losses  result in high frequency attenuation which   expressed in decibels  increases as  w         An ideal step function pulse impressed on the line  appears at the  matched  far end with the shape  shown in Fig  1     The rise time from O to X percent can be  expressed as multiples of T     where To is the O to  50  rise time  Table 1 presents some rise time  conversion factors  an example of the use of these  factors is the following  10  to 90  rise  time    29 0   0 17  To   28 83 To        Fig  T  Step Function Response of Transmission Lines for  Which Decibel Attenuation Varies as the Square Root of  Frequency  The time Ta is defined as the interval measured  from the start of the output pulse to the point at which  Eut 0 5 Ein     In Fig  2  T    is plotted against the delay length in  Nanoseconds                Table 1  Rise Time Conversion Factors    Percent of Pulse Height Rise Time Factor       10 0 17  20 0 28  50 1 0  70 3 1  80 fa  90 29 0  95 110 0       15 30 60 120 a  Cable Length  ns  E    Fig  2  Calculated Variation of 7 with Cable Length  for RG 5BA U     For AG 58A4 U cable whose decibel attenuation varies as   aa   for frequencies between 100 MHz and 1000 MHz  it  is convenient to calculate To by    To   4 0 X 10778 42 2 g   1     where A is the commonly tabulated attenuation at 1000  MHz e
3. arranty should  follow the same procedure and ORTEC will provide a quotation     Damage in Transit  Shipments should be examined immediately upon receipt for evidence of external or concealed damage  The carrier  making delivery should be notified immediately of any such damage  since the carrier is normally liable for damage  in shipment  Packing materials  waybills  and other such documentation should be preserved in order to establish  claims  After such notification to the carrier  please notify ORTEC of the circumstances so that assistance can be  provided in making damage claims and in providing replacement equipment  if necessary     Copyright    2002  Advanced Measurement Technology  Inc  All rights reserved      ORTEC  is a registered trademark of Advanced Measurement Technology  Inc  All other trademarks used herein  are the property of their respective owners                 CONTENTS  WARRANTY ruta ti Id a bla li  SAFETY INSTRUCTIONS AND SYMBOL Sucre clio rt toas iv  SAFETY WARNINGS AND CLEANING INSTRUCTIONS                0c cece eee eee eee tee eee eee V  le DESOGRIPTION ct er eee A A AA ree ET 1  22 OFEGIFICATION Sissi ia 1  Je O O te a erates dere 1  A MAINTE NANG E sets cot Arte etc avedte ac eateet aia nandeneatautenae ace tetantalee et aa E E AAE 3    Oe Ed  Ao siete eh aitedtie enedecing ciara tied abides ee caeh A 4                SAFETY INSTRUCTIONS AND SYMBOLS    This manual contains up to three levels of safety instructions that must be observed in orde
4. ck Diagram of Apparatus Used  in Production Testing  Es       discriminators and the coincidence circuit are  adjusted to the middle of the edge of the decay  curve  i e   50  count rate  The width of this edge  is about 20 ps  that is  changing the adjustable air  line by 20 ps can change the output counting rate  from 100  to 0   When a delay is switched into  the 425A branch  the equivalent length of air line is  introduced into the other branch  lf the delay cable  has the correct length  the count rate will again be  50   if not  the amount of required readjustment  of the variable air line gives the error directly  Both  discriminators operate at 50  amplitude for this  test     The termination of the cable at any realizable  discriminator input is not exactly 50 Q  Commonly  used circuits include the shunt capacity of a tunnel  diode or the base of a fast transistor plus stray  inductances and capacitances  This slight  deviation from perfect termination does not affect  the delay definition appreciably because it is the  same in both branches  Finite test pulse rise time      1 ns  also affects both branches equally  and  so it introduces only second order errors  Also   the air cables are not exactly lossless  but the To  is almost 2 orders of magnitude shorter than for  RG 58A U  so it can be neglected     If a transmission line system were to introduce no   reflections  it would have to have a uniform   impedance i i  p throughout  Since z    LIC  the ratio    of i
5. must pass a stringent set of quality control tests  designed to expose any flaws in materials or workmanship  Permanent records of these tests are maintained for use  in warranty repair and as a source of statistical information for design improvements     Repair Service   If it becomes necessary to return this instrument for repair  it is essential that Customer Services be contacted in  advance of its return so that a Return Authorization Number can be assigned to the unit  Also  ORTEC must be  informed  either in writing  by telephone   865  482 4411  or by facsimile transmission   865  483 2133   of the  nature of the fault of the instrument being returned and of the model  serial  and revision   Rev  on rear panel   numbers  Failure to do so may cause unnecessary delays in getting the unit repaired  The ORTEC standard  procedure requires that instruments returned for repair pass the same quality control tests that are used for new   production instruments  Instruments that are returned should be packed so that they will withstand normal transit  handling and must be shipped PREPAID via Air Parcel Post or United Parcel Service to the designated ORTEC  repair center  The address label and the package should include the Return Authorization Number assigned   Instruments being returned that are damaged in transit due to inadequate packing will be repaired at the sender s  expense  and it will be the sender s responsibility to make claim with the shipper  Instruments not in w
6. nductance to capacitance at each point would  have to be a constant  This cannot be achieved  even for the cable itself  and further deviations  occur when cables must be interconnected and  the pulses routed through switches  At points of  interconnection where excess inductance is  encountered  some small capacitance has been  purposely added  so that the ratio of L C  averaged over the connection is correct   Likewise  the switches have been mounted so  that averaged over the switch gives 50 Q  even  though from point to point there are deviations   Thus reflections occur when the magnitude of the  deviations and the distance over which they  extend become appreciable when compared to  the distance traversed by a pulse during its rise  time  ref  8  For most pulses used in data  acquisition systems in the physics laboratory in  which the rise time is equal to or greater than 1  ns  the reflection introduced at each end of the  each delay cable will be comparable in size to  that incurred when two cables are connected  together by BNC connectors and a BNC union     The temperature coefficient of the delay of the  cables used in the 425A is about 150 ppm   C  within 20   of room temperature     4  MAINTENANCE    The assembly procedures peculiar to the 425A  Delay are considered virtually irreversible     therefore  any warranty problems will be resolved  by replacement of the module                 5  BIBLIOGRAPHY    1  S  Goldman  Transformation Calculus and Electrical Tran
7. ners     CAUTION To prevent moisture inside of the instrument during external cleaning  use only enough liquid    to dampen the cioth or applicator        e Allow the instrument to dry completely before reconnecting it to the power source                 yi                   1    ORTEC MODEL 425A  DELAY    1  DESCRIPTION    The 425A Delay is a single width NIM standard  module that provides for signal delays in 1 ns  steps from 1 7 to 64 7 ns  This is the basic 1 7 ns  instrument delay plus the  switch selected  additional delay  Longer delays may be achieved  by cascading several 425A modules  Input and    Output impedances are 500  The delays are  accomplished by coaxial cables interconnected by  strip line sections  no power is required  Delay  accuracy and definition are discussed in Section 3      Theory        2  SPECIFICATIONS    Input 50 impedance  either polarity  1500 V  maximum BNC connector     Output 50 Q impedance  delay is the sum of IN  switches  BNC connector     Delay Lengths 1  2  4  8  16  and 32 ns  may be  added in any combination     Minimum Delay 1 7 ns  all switches OUT      Delay Accuracy  100 picosecond or  1  for  each delay section used  whichever is greater     Cable Type RG 58A U   Power Required None   Dimensions Standard single width module     1 35 in  wide x 8 714 in  high  per TID 20893   Rev      3  THEORY    Pulses transmitted through coaxial cables suffer  both attenuation and distortion  In the cable used  in the 425A  as in most cables
8. r to avoid personal  injury and or damage to equipment or other property  These are     DANGER Indicates a hazard that could result in death or serious bodily harm if the safety instruction is not  observed     WARNING Indicates a hazard that could result in bodily harm if the safety instruction is not observed     CAUTION Indicates a hazard that could result in property damage if the safety instruction is not  observed     Please read all safety instructions carefully and make sure you understand them fully before attempting to  use this product     In addition  the following symbol may appear on the product     ATTENTION     Refer to Manual    DANGER   High Voltage    Please read all safety instructions carefully and make sure you understand them fully before attempting to  use this product                 SAFETY WARNINGS AND CLEANING INSTRUCTIONS       DANGER Opening the cover of this instrument is likely to expose dangerous voltages  Disconnect the  instrument from all voltage sources while jt is being opened        WARNING Using this instrument in a manner not specified by the manufacturer may impair the    protection provided by the instrument        Cleaning Instructions  To clean the instrument exterior     e Unplug the instrument from the ac power supply   e Remove loose dust on the outside of the instrument with a lint free cloth     e Remove remaining dirt with a lint free cloth dampened in a general purpose detergent and water    solution  Do not use abrasive clea
9. sients  Prentice Hall  New York  1945     2  P  Behrend     Theory of Pulse Technique for Coaxial Cables     Z  Angnew  Physik 5  61  February  1953      3  R  L  Wigington and N  S  Nahman     Transient Analysis of Coaxial Cables Considering Skin Effect     Proc   IRE 45  166  174  February  1957      4  Q  Kerns  F  Kirsten  and C  Winningstad  Pulse Response of Coaxial Cables  revised by R  Kirsten  LRL  Counting Note CC 2 1  Lawrence Radiation Laboratory  University of California  Berkeley  1959     5  W  C  Johnson  Transmission Lines and Networks  McGraw Hill  New York  1950   6  H  H  Skilling  Electric Transmission Lines  McGraw Hill  New York  1951   7  R  Littauer  Pulse Electronics  McGraw Hill  New York  1965     8  Hewlett Packard Company  Time Domain Reflectometry  Application Note 62           
10. xplain the sense in which this definition is  operational  Two counters  scintillation  detect  prompt coincidence gamma rays from a  radioactive source  The source is moved 120 cm  away from one counter and 120 cm closer to the  other  If the cable delay from one counter is  changed by 8ns by use of the 425A  the two  counters will be properly time realigned if the  discriminators associated with each counter are  operated at 50  amplitude  In practice  the  experimenter cannot readily operate at 50   amplitude just to have the cable calibrations  meaningful  but  using Eq   1   it can be seen that  the timing difference between 0  and 50   amplitude is less than 20 ps for a 10 ns length of  RG 58A U  It is in this range of operation that  discriminators are usualy used  If the  discriminator is to be used at a large percentage  of full amplitude or if long delays are to be  achieved at settings other than 50   corrections  can be made by using Fig  1 or Table 1 as a  reference  For the above example  a delay error  of 0 26 ns would result if the discriminator were  operated at the 90  level     Figure 3 shows the block diagram of the  apparatus used in testing the delay cables of the  425A     A fast rising pulse is split into two branches  one  of which is the 425A Delay  The other consists of  sections of high quality rigid air lines with one  adjustable section  The delays between the     See Section 5     Bibliography                       DISC RIMINA TOR    Fig  3  Blo
11. xpressed in db 100 ft  20 to 24 for RG 58A U   and  Fis the length in nanoseconds     Since the rise time is proportional to the square of  the length  if two equal lengths of a given type of  cable are cascaded  the rise time of the  combination is four times the rise time of either  length alone  This is in contrast to the familiar case  of amplifiers of Gaussian frequency response  in  which the rise time varies as the square root of the  number of identical sections  For this reason and  also because the characteristic step function  responses of cables and of Gaussian devices are    so different  the overall rise time of combinations  cannot be calculated from the square root of the  sum of squares of individual rise times  either  with cables alone or with cables combined with  Gaussian elements  Instead  the overall response  of a system with cables and other elements may  be obtained graphically or with convolution  integrals  ref 3    using either step or impulse   obtained from the derivative of the function  plotted in Fig  1  function responses     The above discussion makes it clear that the  delay of a cable cannot be specified unless the  point on the response function is specified  For  the 425A Delay  an operational definition is  chosen  When the required delay has been  selected by any one of the IN switches  the 50   amplitude point will be delayed by an amount  equal to the delay that would be effected by  lossless delay line  One example will serve to  e
    
Download Pdf Manuals
 
 
    
Related Search
    
Related Contents
Franke FHM 302 2E XS  NEC Express5800/120Li User's Guide  Quartz Chronographs User`s Manual  Kenroy Home 32692WDG Installation Guide    Copyright © All rights reserved. 
   Failed to retrieve file