polibuda said:
Thank you for help, but i have still problem with calculating the second electric intesity. Could you help me?
For this problem you don't have to calculate the second field intensity. You just have to be mindful that there are limitations to ##E = \frac{\Delta V}{\Delta d}## and use another approach. You don't have to find the second field intensity but you do have to be careful of assuming that they are the same at different equipotential surfaces.
Are you familiar with the equation for a positive charge
##E = \frac{Q}{4 \pi \epsilon_0 r^2}##?
and
##V = \frac{Q}{4 \pi \epsilon_0 r}##?
Given that we have ##E = 10^4 \frac{V}{m}## at ##r = 0.05 \text{ m}## we can solve for ##Q## (Do this part on your own and tell me what you get)
Plug your answer for ##Q## into the following and tell me what you get.
##V \left( r = 0.05 \text{ m} \right) = \frac{Q}{4 \pi \epsilon_0 \left( 0.05 \right)} ##
taking your previous answer for V
then solve the equations
##V \pm 100 = \frac{Q}{4 \pi \epsilon_0 r_2}##
for ##r_2## that will tell you the distance from the original point charge to the second equipotential surface.
Like I said, depending on what level you're at the answers ##4 \text{cm}## and ##6 \text{cm}## may be right.