Killing Cancer

Description

>Top


ID:(1491, 0)



DNA chain

Image

>Top


ID:(2702, 0)



Damage by Ionizing Radiation

Description

>Top


ID:(1492, 0)



Direct Method

Description

>Top


ID:(240, 0)



oncology005

Image

>Top


![oncology005](showImage.php)

oncology005

ID:(7374, 0)



Indirect Method

Description

>Top


ID:(241, 0)



oncology006

Image

>Top


![oncology006](showImage.php)

oncology006

ID:(7375, 0)



oncology016

Image

>Top


![oncology016](showImage.php)

oncology016

ID:(7385, 0)



oncology017

Image

>Top


![oncology017](showImage.php)

oncology017

ID:(7386, 0)



oncology018

Image

>Top


![oncology018](showImage.php)

oncology018

ID:(7387, 0)



Probability to Impact the Core

Description

>Top


ID:(239, 0)



Probability to Impact Chromosome

Description

>Top


ID:(847, 0)



Probability to Impact DNA

Description

>Top


ID:(848, 0)



Probability of DNA Damage

Description

>Top


ID:(849, 0)



Types of DNA Damage

Image

>Top


ID:(1722, 0)



Electron LET

Description

>Top


ID:(1503, 0)



Examples of LET

Description

>Top


ID:(1486, 0)



Situation in Tissue

Description

>Top


ID:(1502, 0)



Survival of Cells

Image

>Top


ID:(2708, 0)



Camino medio por una Esfera

Equation

>Top, >Model


El camino medio que recorre una partícula por una esfera se puede calcular primero considerando el camino medio en un disco de radio $r$ en el plano $y-z$ lo que es

$\bar{r}_2=\displaystyle\frac{2\int_0^r\sqrt{r^2-z`2}dz}{\int_0^r dz}=\displaystyle\frac{\pi r}{2}$

para luego promediar este valor en el eje $x$ considerando que la cantidad de puntos es proporcional a la altura de la esfera por lo que

$\bar{r}_3=\displaystyle\frac{\int_0^r\sqrt{r^2-x^2}\displaystylefrac{\sqrt{r^2-x^2}\pi}{2}dx}{\int_0^r \sqrt{r^2-x^2}dx}=\displaystyle\frac{\pi r^2}{2}=\displaystyle\frac{4}{3\pi}r$

lo que equivale a aproximadamente $42\%$ del radio $r$.

ID:(7400, 0)