- #36
voko
- 6,054
- 391
That is probably all correct, but I do not understand where that gets you. What is the purpose of those calculations?
Here is how you could employ the method of #14. I will use the data from the original excel sheet, namely ##v_1 = 70 \ \text{km/h} = 19.4 \ \text{m/s}, v_2 = 60.3 \ \text{km/h} = 16.8 \ \text{m/s}, v_3 = 51.5 \ \text{km/h} = 14.3 \ \text{m/s} ##, uniform ##10 \ \text{s}## time interval.
The basic equation in #14 was ##\arctan \alpha v_{1f} - \arctan \alpha v_{1i} = \arctan \alpha v_{2f} - \arctan \alpha v_{2i} ##, which in this case simplifies to $$ 2 \arctan \alpha v_2 - \arctan \alpha v_1 - \arctan \alpha v_3 = 0 $$ Cheating, I get ## \alpha = 0.022931 ##. To determine ##a##: $$ a = \frac 1 {\alpha T} (\arctan \alpha v_2 - \arctan \alpha v_1) = \frac 1 {\alpha T} (\arctan \alpha v_3 - \arctan \alpha v_2) $$ and I get $$ \frac 1 {\alpha T} (\arctan \alpha v_2 - \arctan \alpha v_1) = -0.221769 $$ and $$ \frac 1 {\alpha T} (\arctan \alpha v_3 - \arctan \alpha v_2) = -0.221769 $$ which I call pretty good agreement :)
Given $$ a = - \frac R m = - \frac {mgC_r}{m} = -gC_r $$ and $$ \alpha = \sqrt {\frac { \rho A }{2mg}} \sqrt {\frac { C_d }{C_r}}$$ we should have $$ C_r = -{a \over g}$$ and $$ C_d = {2 mg \over \rho A} \alpha^2 C_r $$ From the constants in the original sheet, I obtain ## C_r = - 0.023 ## and ## C_d = 0.083 ##, which differ quite significantly from the results in the spreadsheet.
Here is how you could employ the method of #14. I will use the data from the original excel sheet, namely ##v_1 = 70 \ \text{km/h} = 19.4 \ \text{m/s}, v_2 = 60.3 \ \text{km/h} = 16.8 \ \text{m/s}, v_3 = 51.5 \ \text{km/h} = 14.3 \ \text{m/s} ##, uniform ##10 \ \text{s}## time interval.
The basic equation in #14 was ##\arctan \alpha v_{1f} - \arctan \alpha v_{1i} = \arctan \alpha v_{2f} - \arctan \alpha v_{2i} ##, which in this case simplifies to $$ 2 \arctan \alpha v_2 - \arctan \alpha v_1 - \arctan \alpha v_3 = 0 $$ Cheating, I get ## \alpha = 0.022931 ##. To determine ##a##: $$ a = \frac 1 {\alpha T} (\arctan \alpha v_2 - \arctan \alpha v_1) = \frac 1 {\alpha T} (\arctan \alpha v_3 - \arctan \alpha v_2) $$ and I get $$ \frac 1 {\alpha T} (\arctan \alpha v_2 - \arctan \alpha v_1) = -0.221769 $$ and $$ \frac 1 {\alpha T} (\arctan \alpha v_3 - \arctan \alpha v_2) = -0.221769 $$ which I call pretty good agreement :)
Given $$ a = - \frac R m = - \frac {mgC_r}{m} = -gC_r $$ and $$ \alpha = \sqrt {\frac { \rho A }{2mg}} \sqrt {\frac { C_d }{C_r}}$$ we should have $$ C_r = -{a \over g}$$ and $$ C_d = {2 mg \over \rho A} \alpha^2 C_r $$ From the constants in the original sheet, I obtain ## C_r = - 0.023 ## and ## C_d = 0.083 ##, which differ quite significantly from the results in the spreadsheet.