Respuesta :
Answer:
[tex]A) \,K.E=1.405\times 10^{-20}J[/tex]
[tex]B)\,r_f=0.268\,m[/tex]
Explanation:
[tex]Charge\,\,density=\lambda=6\times 10^{-12}C/n\\\\Mass\,\, of \,\,proton=m_p=1.67\times 10^{-27}kg\\\\charge\,\, of\,\, proton=q_p=1.609\times 10^{-19}C\\\\r=12\,cm=0.12\, m\\\\v=4.103\times 10^{3}m/s[/tex]
A) Initial kinetic energy of proton
[tex]K.E=\frac{1}{2}m_pv^2\\\\K.E=1.405\times 10^{-20}J[/tex]
B) How close does the proton get to the line of charge?
Potential energy and kinetic energy are related as:
[tex]K_i+U_i=K_f+U_f\\\\U_f-U_i=K_i-K_f\\\\q(V_f-V_i)=1.40\times 10^{-20}\\\\V_f-V_i=0.087--(1)\\[/tex]
Change in voltage is
[tex]V_f-V_i=\frac{\lambda}{2\pi \epsilon_o}ln\frac{r_f}{r_i}\\\\ln|\frac{r_f}{r_i}|=(0.087)(\frac{2\pi \epsilon_o}{\lambda})\\\\ln|\frac{r_f}{r_i}|==0.8059\\\\\frac{r_f}{r_i}=2.24\\\\r_f=(2.24)(.12)\\\\r_f=0.268 m[/tex]
As the proton approaches the line of charge:
(a) The initial kinetic energy of the proton is 1.4×10⁻²⁰J
(b) Distance of closest approach is 0.266m
Calculating the distance of the closest approach:
Given that the linear charge density of the line is λ = 6×10⁻¹² C/m
mass of the proton, m = 1.67×10⁻²⁷kg
charge on proton, q = 1.6×10⁻¹⁹ C
initial distance of the proton, r = 12cm = 0.12m
velocity of the proton, v = 4.1×10³ m/s
(a) Initial kinetic energy of the proton is given by:
KE = ¹/₂mv²
KE = 0.5×(1.67×10⁻²⁷)×(4.1×10³)²
KE = 1.4×10⁻²⁰J
(b) When the proton is closest to the line of charge, its velocity is zero, so according to the conservation of energy, all the kinetic energy is converted into potential energy
The change in potential energy due to linear charge density is given by:
[tex]\Delta U=\frac{\lambda q}{4\pi\epsilon_0}\ln\frac{r'}{r}[/tex]
where r' is the final position
since ΔU = KE = 1.4×10⁻²⁰J
[tex]1.4\times10^{-20}=9\times10^9\times6\times10^{-12}\times1.67\times10^{-27}\ln\frac{r'}{0.12}\\\\\ln\frac{r'}{0.12}=0.8\\\\\frac{r'}{0.12}=2.22[/tex]
r' = 0.266m
So, the proton gets as close as 0.266m to the line of charge.
Learn more about linear charge density :
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