Dytran 1051C Скачать руководство пользователя страница 3

Rev B,  ECN 12897, 08/18/16 
 

 

  

 -q 

 

  V

 =  --------                    (Eq 1) 

 

 

C

f

 

 
Where:  
 

V

 is the output voltage (Volts) 

 

q   is the input charge, (pC) 

 

C

f

  is the feedback capacitor, (pF) 

 
 

This means that the sensitivity of the charge 

amplifier is determined by the value of the feedback 
capacitor only. Since the output voltage is fed back 
to the summing junction of the amplifier (the input 
terminal) the virtual input impedance is extremely 
high which means that the charge signal generated 
by the quartz crystals will not be drained away by 
the measuring device. 
 

SIGNAL POLARITY 
 
 

Compressive forces on these sensors (see 

Figure 1) produce negative-going output signals. 
This is because most charge amplifiers are inverting 
amplifiers and the output signal from the charge 
amplifier will be positive going for compressive 
loads. This is conventional. 
 
 

By the same token, tension loads on the 

1051C will produce positive-going output signals. 
 

SENSITIVITY

 

 
 

The nominal charge sensitivity of Model 

1051C is -18 pC/Lb. 
 

CHARGE AMPLIFIER SELECTION 

 
 

Dytran manufactures many different types of 

charge amplifiers to suit the needs of most any 
measurement requirement from the larger laboratory 
type Model 4165 which features ranging and filtering 
plus standardization to the miniature in-line types 
4751 and 4705 which adapt the 1051C to LIVM 
operation with constant current power units. 
 

For laboratory measurements, the 4165 is 

recommended and for field use, the dedicated 
sensitivity n-line charge amplifiers may be a better 
choice. 
 
 

Consult the factory for recommendations on 

the best type of charge amplifier for your 
measurement needs. 
 
 
 
 

INSTALLATION

 

 
 

Refer to outline/installation drawing 127-

1051C, supplied with this guide. 
 
 

To mount model 1051C, it is necessary to 

prepare a flat smooth mounting surface of 5/8” 
minimum diameter. The surface should be flat to 
.0005 TIR for best results. 
 
 

The surrounding area must provide for room 

to connect the cable to the 10-32 connector at the 
end of the radial connector housing. Drill and tap a 
1/4-28 hole to accept the model 6204 1/4-28 
mounting stud.  Thread in the mounting stud 
(supplied) to secure the 1051C to its mounting 
surface. 
 
 

Before mounting the 1051C, thread the 

sensor into the mounting port and examine the fit of 
the mounting surfaces. They must meet parallel, i.e., 
a wedge must 

not

 be formed between these 

surfaces. Also, at this time, inspect the mating 
surfaces for foreign particles, which may become 
lodged between these surfaces and clean if 
necessary. It is important that the mating surfaces 
meet squarely and intimately with no particles of 
foreign matter of any kind included between them. 
Foreign particles included between mating surfaces 
could damage the sensor and/or modify the 
sensitivity of the sensor. 
 
 

When you are satisfied that the surfaces are 

square and clean, place a thin layer of silicone 
grease on one of the surfaces and thread the force 
sensor place, torquing it in place with 25 to 30 Lb-
inches of torque to secure. 
 
 

For most impact applications, the Model 

6210S (steel) impact cap will be utilized. This cap is 
threaded into the platen (top surface of the force 
sensor). Thread this cap securely into the tapped 
hole in the platen, again inspecting for foreign 
particles between mating surfaces and clean if 
necessary. For more permanent installations, 
thread-locking compounds may be used to secure 
the installation. Use these compounds sparingly. 
 
 

For a slightly higher resonant frequency, the 

aluminum cap, Model 6210A, may be a better choice 
in some applications. 
 
 

Connect the sensor to the charge amplifier 

using Series 6010AXX cable (10-32 to 10-32) or 
Series 6011AXX (10-32 to BNC plug), depending on 
the connector called for by the power unit. Tighten 

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