ScienTECH 380401 Setup And Operating Procedures Download Page 6

 

6

Initial Voltage Interpolation: 

A method used to eliminate the tedious numerical integration task is to project the thermal decay envelope on to 
the voltage axis, determine the 1/e decay time constant T, and estimate the total energy value (E): 
 

E = (V

o

/S) x T 

The change from thermal absorption to thermal transport phenomena near the peak causes difficulty in 
accurately projecting the envelope on to the voltage axis introducing an error, dV

o

. Further, the determination of 

the time constant T, introduces another error, dT. The total error is the sum of the two errors. 
 

dE = (V

o

/S)dT + (T/S)dV

o

 

The difficulty in eliminating the potential error makes this method typically less accurate than numerical 
integration, but much faster in application. 
 

Peak Voltage Estimate: 

The peak voltage method requires using an independent determination of total energy and referencing it back to 
the peak voltage value, V

p

 
For a given pulse, use the numerical integration method to obtain E.  Note the peak voltage, V

p

. Compute the 

value, F 
 

F = E/V

p

 

 
For the next pulse compute the total energy:       E = F x V

p

 

 
The error in using this method yields:       dE = FdV

p

 + V

p

dF 

 
The accuracy of this measurement depends upon the error in the original calibration, dF, and the error in the 
peak voltage dV

p

.  A careful numerical integration yields a value for dF near zero.  The value of dV

p

 can be 

minimized by maintaining the geometry of the system (i.e. beam intensity, beam profile, wavelength and 
environment) during operation to be the same as during calibration.  Under controlled circumstances, the peak 
method accuracy usually falls between the numerical integration and initial voltage interpolation methods. 
 

Calibration of Large Aperture Calorimeters: 

A.

 

Refer to Figure 1.  Connect a DVM to the white jacks of the calorimeter. 

B.

 

Measure the resistance of the substitution heater making sure to subtract the resistance of the patch 
cables from the total resistance measurement. 

Note:  When measuring the substitution heater resistance of a 200 mm calorimeter, R1 and R2 

must be connected together in series. 

Compare this resistance to Rc in the calibration data in the front of the manual.  The two should agree 
within 2%.  If not, contact Scientech. 

C.

 

Calculate the voltage equivalent to laser power using the following formula: 

V = (R

c

 x C x W)

1/2

 

where: 
 

V = voltage applied to the heater coil 

 

R

c

 = substitution heater resistance from step B 

 

C = Cal coefficient 

360401 = 1.018 

360801 = 1.000 

 

 

 

380401 = 0.974 

380801 = 1.008 

 

 

 

380402 = 1.024 

380802 = 1.008 

 

 

 

384UV5 = 1.021 

388UV5 = 1.002 

 

W = desired laser power in watts 

D.

 

Connect the DVM to the calorimeter’s DIN connector. 

E.

 

Apply the calculated voltage (V) to the electrical substitution heater. 

Summary of Contents for 380401

Page 1: ...100mm and 200mm Calorimeters Setup and Operating Procedures PN11434C ...

Page 2: ...ertification 3 Environmental Requirements 3 Unpacking and Set Up 4 Cable Requirements 4 Calorimeter Operation Without an Indicator 4 Operation of Large Aperture Calorimeters with a Digital Volt Meter 4 Operation of Large Aperture Calorimeters with an Analog Chart Recorder 5 Calorimeter Response 5 Numerical Integration 5 Initial Voltage Interpolation 6 Peak Voltage Estimate 6 Calibration of Large A...

Page 3: ...1GW cm2 532 nm 27GW cm2 355 nm 530MW cm2 266nm Note 5 384UV5 388UV5 Repetitive pulses 101MW cm2 355nm Single pulses 3 5GW cm2 355nm Note 6 380801 45GW cm2 1064 nm 35 5GW cm2 532 nm 13 5GW cm2 355 nm 265MW cm2 266nm Note 7 360401 360801 Max J cm2 1000 x pulse width 1 2 to a maximum of 200J cm2 Note 8 380401 Repetitive pulses 3 7J cm2 1064nm 2 9J cm2 532nm 1J cm2 355nm 20mJ cm2 266nm Single pulses 7...

Page 4: ... REQUIREMENTS Refer to Figure 1 The output of the calorimeter is connected directly to the DVM or chart recorder Large aperture calorimeters do not require any power The voltage output is on pin 1 of the DIN connector and should be connected to the positive side of the DVM or chart recorder Ground is on pin 3 and should be connected to the negative side Pin 2 is not used Figure 1 100mm and 200mm c...

Page 5: ... E W t dt 0 The following methods may be used to compute the total integrated energy Numerical Integration Finding the area under the curve in figure 7 is the equivalent procedure for determining pulse energy Choose an appropriate time interval dt and perform the summation N N E Wixdt dt S Vi I 1 i 1 The error caused by this procedure is N dE dt S Σ dVi i 1 The error in theory is only dependent up...

Page 6: ... in the peak voltage dVp A careful numerical integration yields a value for dF near zero The value of dVp can be minimized by maintaining the geometry of the system i e beam intensity beam profile wavelength and environment during operation to be the same as during calibration Under controlled circumstances the peak method accuracy usually falls between the numerical integration and initial voltag...

Page 7: ...foregoing warranty is in lieu of all other warranties expressed or implied including but not limited to any implied warranty of merchantability fitness or adequacy for any special incidental or consequential damages whether in contract tort or otherwise RETURNED GOODS PROCEDURE Should it become necessary to return any item to Scientech for any reason please contact our Product Service Department a...

Page 8: ...tion is to reuse the equipment in its entirety 2 Where the equipment can not be reused in its entirety priority should be given to reuse of its subassemblies and components 3 Where reuse is not appropriate electrical and electronic equipment including batteries should be recycled according to local ordinances It should never be mixed with municipal waste ...

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