Comparing With Whitney Rates - Revision history

Vanwdani at 20:32, 28 March 2018

2018-03-28T20:32:19Z

Vanwdani at 20:30, 28 March 2018

2018-03-28T20:30:29Z

Vanwdani at 15:48, 14 March 2018

2018-03-14T15:48:07Z

Vanwdani at 15:47, 14 March 2018

2018-03-14T15:47:45Z

Vanwdani at 15:44, 14 March 2018

2018-03-14T15:44:11Z

Vanwdani at 15:39, 14 March 2018

2018-03-14T15:39:52Z

Vanwdani at 15:30, 14 March 2018

2018-03-14T15:30:18Z

Vanwdani at 19:02, 12 March 2018

2018-03-12T19:02:42Z

Vanwdani at 19:00, 12 March 2018

2018-03-12T19:00:12Z

Vanwdani at 03:21, 12 February 2018

2018-02-12T03:21:04Z

← Older revision		Revision as of 20:32, 28 March 2018
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	Using just the scattered particles, for the total time run,		Using just the scattered particles, for the total time run,
−	<center><math>\sigma=\frac{ N_{scattered}}{ N_{incident}}\frac{1}{\rho \ell}\Rightarrow N_{incident}=\frac{t\ N_{scattered}}{~~\Delta t~~\sigma \rho \ell}=\frac{~~0.0954\times 10^{-3}\ s\ \times~~ 1000000}{~~250 \times 10^{-9}\ s \times~~ .078\cdot 2.11\times 10^{-1}}</math></center>	+	<center><math>\sigma=\frac{ N_{scattered}}{ N_{incident}}\frac{1}{\rho \ell}\Rightarrow N_{incident}=\frac{ N_{scattered}}{\sigma \rho \ell}=\frac{ 1000000}{ .078\cdot 2.11\times 10^{-1}}\approx 6\times 10^7\ incident</math></center>

@@ Line 112: / Line 112: @@
 <center><math>N_{Moller} =R_{Moller}\cdot t_{simulated}=\frac{9.97\times 10^{9}Moller}{s} \cdot 9.54\times 10^{-5} s=951138\ Moller</math></center>
+If we view the window for each region as how many events can be detected per second
 <center><math>\sigma=\frac{ t\ N_{scattered}}{\Delta t N_{incident}}\frac{1}{\rho \ell}\Rightarrow N_{incident}=\frac{t\ N_{scattered}}{\Delta t\sigma \rho \ell}=\frac{0.0954\times 10^{-3}\ s\ \times 1000000}{250 \times 10^{-9}\ s \times .078\cdot 2.11\times 10^{-1}}\approx 6\times 10^7\ incident \times 380 \approx 2\times 10^{10}</math></center>

← Older revision		Revision as of 15:48, 14 March 2018
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−	<center><math>\sigma=\frac{ t\ N_{scattered}}{\Delta t N_{incident}}\frac{1}{\rho \ell}\Rightarrow N_{incident}=\frac{t\ N_{scattered}}{\Delta t\sigma \rho \ell}=\frac{0.0954\times 10^{-3}\ s\ \times 1000000}{250 \times 10^{-9}\ s \times .078\cdot 2.11\times 10^{-1}}\approx 6\times 10^7\ incident \times 380 \approx 2\times 10^10</math></center>	+	<center><math>\sigma=\frac{ t\ N_{scattered}}{\Delta t N_{incident}}\frac{1}{\rho \ell}\Rightarrow N_{incident}=\frac{t\ N_{scattered}}{\Delta t\sigma \rho \ell}=\frac{0.0954\times 10^{-3}\ s\ \times 1000000}{250 \times 10^{-9}\ s \times .078\cdot 2.11\times 10^{-1}}\approx 6\times 10^7\ incident \times 380 \approx 2\times 10^{10}</math></center>



	<center><math>\left ( \frac{Number\ of\ hits}{Moller\ electron}\right ) \left (\frac{Moller\ electrons}{incidents\ electron} \right) \left (\frac{incident\ electrons}{sec} \right )</math></center>		<center><math>\left ( \frac{Number\ of\ hits}{Moller\ electron}\right ) \left (\frac{Moller\ electrons}{incidents\ electron} \right) \left (\frac{incident\ electrons}{sec} \right )</math></center>

← Older revision		Revision as of 15:47, 14 March 2018
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−	<center><math>\sigma=\frac{ t\ N_{scattered}}{\Delta t N_{incident}}\frac{1}{\rho \ell}\Rightarrow N_{incident}=\frac{t\ N_{scattered}}{\Delta t\sigma \rho \ell}=\frac{0.0954\times 10^{-3}\ s\ \times 1000000}{250 \times 10^{-9}\ s \times .078\cdot 2.11\times 10^{-1}}\approx 6\times 10^7\ incident </math></center>	+	<center><math>\sigma=\frac{ t\ N_{scattered}}{\Delta t N_{incident}}\frac{1}{\rho \ell}\Rightarrow N_{incident}=\frac{t\ N_{scattered}}{\Delta t\sigma \rho \ell}=\frac{0.0954\times 10^{-3}\ s\ \times 1000000}{250 \times 10^{-9}\ s \times .078\cdot 2.11\times 10^{-1}}\approx 6\times 10^7\ incident \times 380 \approx 2\times 10^10</math></center>



	<center><math>\left ( \frac{Number\ of\ hits}{Moller\ electron}\right ) \left (\frac{Moller\ electrons}{incidents\ electron} \right) \left (\frac{incident\ electrons}{sec} \right )</math></center>		<center><math>\left ( \frac{Number\ of\ hits}{Moller\ electron}\right ) \left (\frac{Moller\ electrons}{incidents\ electron} \right) \left (\frac{incident\ electrons}{sec} \right )</math></center>

← Older revision		Revision as of 15:44, 14 March 2018
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−	<center><math>\sigma=\frac{N_{scattered}}{N_{incident}}\frac{1}{\rho \ell}\Rightarrow N_{incident}=\frac{N_{scattered}}{\sigma \rho \ell}=\frac{1000000}{.078\cdot 2.11\times 10^{-1}}\approx 6\times 10^7\ incident </math></center>	+	<center><math>\sigma=\frac{ t\ N_{scattered}}{\Delta t N_{incident}}\frac{1}{\rho \ell}\Rightarrow N_{incident}=\frac{t\ N_{scattered}}{\Delta t\sigma \rho \ell}=\frac{0.0954\times 10^{-3}\ s\ \times 1000000}{250 \times 10^{-9}\ s \times .078\cdot 2.11\times 10^{-1}}\approx 6\times 10^7\ incident </math></center>



	<center><math>\left ( \frac{Number\ of\ hits}{Moller\ electron}\right ) \left (\frac{Moller\ electrons}{incidents\ electron} \right) \left (\frac{incident\ electrons}{sec} \right )</math></center>		<center><math>\left ( \frac{Number\ of\ hits}{Moller\ electron}\right ) \left (\frac{Moller\ electrons}{incidents\ electron} \right) \left (\frac{incident\ electrons}{sec} \right )</math></center>

← Older revision		Revision as of 15:39, 14 March 2018
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	<center><math>N_{Moller} =R_{Moller}\cdot t_{simulated}=\frac{9.97\times 10^{9}Moller}{s} \cdot 9.54\times 10^{-5} s=951138\ Moller</math></center>		<center><math>N_{Moller} =R_{Moller}\cdot t_{simulated}=\frac{9.97\times 10^{9}Moller}{s} \cdot 9.54\times 10^{-5} s=951138\ Moller</math></center>
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← Older revision		Revision as of 15:30, 14 March 2018
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−	<center><math>\sigma=\frac{N_{~~events~~}}{N_{incident}}\frac{1}{\rho \ell}\Rightarrow N_{incident}=\frac{N_{~~events~~}}{\sigma \rho \ell}=\frac{~~951138~~}{.~~075~~\cdot 2.11\times 10^{-1}}=6\times 10^7\ incident </math></center>	+	<center><math>\sigma=\frac{N_{scattered}}{N_{incident}}\frac{1}{\rho \ell}\Rightarrow N_{incident}=\frac{N_{scattered}}{\sigma \rho \ell}=\frac{1000000}{.078\cdot 2.11\times 10^{-1}}\approx 6\times 10^7\ incident </math></center>



	<center><math>\left ( \frac{Number\ of\ hits}{Moller\ electron}\right ) \left (\frac{Moller\ electrons}{incidents\ electron} \right) \left (\frac{incident\ electrons}{sec} \right )</math></center>		<center><math>\left ( \frac{Number\ of\ hits}{Moller\ electron}\right ) \left (\frac{Moller\ electrons}{incidents\ electron} \right) \left (\frac{incident\ electrons}{sec} \right )</math></center>

← Older revision		Revision as of 19:02, 12 March 2018
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	For a 5cm target of LH2:		For a 5cm target of LH2:

−	<center><math>\rho_{target}\times l_{target}=\frac{70.85 kg}{1 m^3}\times \frac{1 mole}{2.02 g} \times \frac{1000g}{1 kg} \times \frac{6.022\times10^{23} molecules\ LH_2}{1 mole} \frac{2 atoms}{1\ molecule\ LH_2} \times \frac{1m^3}{(100 cm)^3} \times \frac{5 cm}{ }=\frac{2.11\times 10^{23}}{cm^2} \times \frac{10^{-23} cm^{2}}{barn}=0.211 barns^{-1}</math></center>	+	<center><math>\rho_{target}\times l_{target}=\frac{70.85 kg}{1 m^3}\times \frac{1 mole}{2.02 g} \times \frac{1000g}{1 kg} \times \frac{6.022\times10^{23} molecules\ LH_2}{1 mole} \frac{2 atoms}{1\ molecule\ LH_2} \times \frac{1m^3}{(100 cm)^3} \times \frac{5 cm}{ }=\frac{2.11\times 10^{23}}{cm^2} \times \frac{1^{-24} cm^{2}}{barn}=0.211 barns^{-1}</math></center>

← Older revision		Revision as of 19:00, 12 March 2018
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	For a 5cm target of LH2:		For a 5cm target of LH2:

−	<center><math>\rho_{target}\times l_{target}=\frac{70.85 kg}{1 m^3}\times \frac{1 mole}{2.02 g} \times \frac{1000g}{1 kg} \times \frac{6.022\times10^{23} molecules\ LH_2}{1 mole} \frac{2 atoms}{1\ molecule\ LH_2} \times \frac{1m^3}{(100 cm)^3} \times \frac{5 cm}{ }=\frac{2.11\times 10^{23}}{cm^2} \times \frac{10^{-24} cm^{2}}{barn}=2.~~11\times 10^{-1}\~~ barns^{-1}</math></center>	+	<center><math>\rho_{target}\times l_{target}=\frac{70.85 kg}{1 m^3}\times \frac{1 mole}{2.02 g} \times \frac{1000g}{1 kg} \times \frac{6.022\times10^{23} molecules\ LH_2}{1 mole} \frac{2 atoms}{1\ molecule\ LH_2} \times \frac{1m^3}{(100 cm)^3} \times \frac{5 cm}{ }=\frac{2.11\times 10^{23}}{cm^2} \times \frac{10^{-23} cm^{2}}{barn}=0.211 barns^{-1}</math></center>

← Older revision		Revision as of 03:21, 12 February 2018
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		+	<center><math>\textbf{Navigation}</math></center>
		+
		+	<center>
		+	[[Lorentz_Transformation_to_Lab_Frame\|<math>\vartriangleleft </math>]]
		+	[[VanWasshenova_Thesis#Weighted_Isotropic_Distribution_in_Lab_Frame\|<math>\triangle </math>]]
		+	[[CED_Verification_of_DC_Angle_Theta_and_Wire_Correspondance\|<math>\vartriangleright </math>]]
		+	</center>
		+
	Using the values from Whitney:		Using the values from Whitney: