91 lines
1.9 KiB
Markdown

| Voltage | Count |
| ------- | ------- |
| 800 | 5499 |
| 600 | nothing |
| 650 | 4860 |
| 675 | 4504 |
| 700 | 4803 |
| 725 | 5007 |
| 750 | 5094 |
| 775 | 5326 |
| 800 | 5484 |
| 825 | 5443 |
| 850 | 5715 |
| 875 | 5892 |
| 900 | 5801 |
| 925 | 6009 |
| 950 | 6045 |
| 975 | 6114 |
| 1000 | 6298 |
| 1025 | 6392 |
| 1050 | 6452 |
| 1075 | 6641 |
| 1200 | 10089 |
Our samples were pretty diluted
1 Minute Count at 925 volts 2cm
~17k
1 minute count at 925 volts 1cm
28740 counts
Right half only 1 minute count at 925 volts 1cm R1
15460 counts
Both halves 1 minute count at 925 volts 1cm R12
28966 counts
Left half only 1 minute count at 925 voltes 1cm R2
15257 counts
Question 3.1 we may not really have to do
Exercise 3.4
238.9 microseconds between pulses observed
calculated was 236.2
Now with the blank disk
measurements in script
removing both halves
background count is 32
```
danesabo@danesabo-laptop:~/Projects/class_work/NUCE_2113$ python3 quick_maths.py
t_d = 2.362e-04
perc deadtime =11.401
t_d = 2.115e-04
perc deadtime =10.317
danesabo@danesabo-laptop:~/Projects/class_work/NUCE_2113$ cat quick_maths.py
#rad disk
R_1=15460
R_12 = 28966
R_2 = 15257
R_b = 0
X = R_1*R_2 - R_b*R_12
Y = R_1*R_2*(R_12+R_b) - R_b*R_12*(R_1+R_2)
Z = Y*(R_1+R_2 - R_12-R_b)/X**2
T_d = X*(1-(1-Z)**(1/2))/Y *60
print(f't_d = {T_d:.3e}')
#Exercise 3.1
print(f'perc deadtime ={T_d*R_12/60*100:.3f}')
#blank disk
R_1=15280
R_12 = 29273
R_2 = 15585
R_b = 0
X = R_1*R_2 - R_b*R_12
Y = R_1*R_2*(R_12+R_b) - R_b*R_12*(R_1+R_2)
Z = Y*(R_1+R_2 - R_12-R_b)/X**2
T_d = X*(1-(1-Z)**(1/2))/Y *60
print(f't_d = {T_d:.3e}')
#Exercise 3.1
print(f'perc deadtime ={T_d*R_12/60*100:.3f}')
```
- [x] make tasks for what needs done for this #NUCE2113 ⏳ 2025-02-05 📅 2025-02-05 ✅ 2025-02-10