To find the point between two charges where the electric field is zero, you can use the principle of superposition.
Assume you have two point charges: \( q_1 \) and \( q_2 \). The electric field \( E \) due to a point charge is given by:
\[
E = k \frac{|q|}{r^2}
\]
where \( k \) is Coulomb's constant, \( q \) is the charge, and \( r \) is the distance from the charge.
### Steps to find the zero electric field point:
1. **Identify the charges**: Assume \( q_1 \) is positive and \( q_2 \) is negative (or vice versa).
2. **Determine the region**: The point where the electric field is zero will be along the line connecting the two charges. You should look for a point between them, but it could also be outside, depending on the magnitudes and signs of the charges.
3. **Set up the equation**: If the charges are \( q_1 \) and \( q_2 \) separated by a distance \( d \), let \( x \) be the distance from \( q_1 \) to the point where the electric field is zero. The distance from \( q_2 \) to that point would then be \( d - x \).
4. **Write the electric fields**: The electric fields due to each charge at that point will be:
- Due to \( q_1 \): \( E_1 = k \frac{|q_1|}{x^2} \)
- Due to \( q_2 \): \( E_2 = k \frac{|q_2|}{(d - x)^2} \)
5. **Set them equal**: For the electric field to be zero, the magnitudes must be equal:
\[
k \frac{|q_1|}{x^2} = k \frac{|q_2|}{(d - x)^2}
\]
Simplifying this gives:
\[
\frac{|q_1|}{x^2} = \frac{|q_2|}{(d - x)^2}
\]
6. **Cross-multiply and solve for \( x \)**:
\[
|q_1| (d - x)^2 = |q_2| x^2
\]
Expanding and rearranging will lead to a quadratic equation in \( x \).
7. **Evaluate possible solutions**: Depending on the relative magnitudes of the charges, you may find that the zero field point lies either between the charges or outside of them.
### Conclusion
To determine the specific location, you will need the values of \( q_1 \) and \( q_2 \). If they are of opposite signs, there will definitely be a point between them where the field is zero. If they are both positive or both negative, there won't be a point between them; instead, look outside.