Two charged conducting spheres of radii aand bare connected to each ot...
Let q1 and q2 be the charges and C1 and C2 be the capacitance of two spheres
The charge flows from the sphere at higher potential to the other at lower potential, till their potentials becomes equal.
After sharing, the charges on two spheres would be
q1/q2 = C1V/C2V…(i)
Also C1C2 = ab…(ii)
From (i) q1/q2 = a/b
Ratio of surface charge on the two spheres
σ1/σ2 = q1/4πa2⋅4πb2/q2 = q1/q2⋅b2/a2 = b/a(using(ii)
∴ The ratio of electric fields at the surfaces of two spheres E1/E2 = σ1/σ2 = b/a
Two charged conducting spheres of radii aand bare connected to each ot...
Given information:
- Two charged conducting spheres of radii a and b are connected to each other by a wire.
To find:
- The ratio of electric fields at the surfaces of two spheres.
Solution:
Step 1: Understanding the situation
- We have two charged conducting spheres of different radii connected by a wire.
- Since the spheres are conducting, the charges on their surfaces will distribute evenly.
- Let the charge on the first sphere be q1 and the charge on the second sphere be q2.
Step 2: Electric field at the surface of a sphere
- The electric field at the surface of a sphere is given by the equation E = k * (q/r^2), where k is the electrostatic constant, q is the charge on the sphere, and r is the radius of the sphere.
- Therefore, the electric field at the surface of the first sphere is E1 = k * (q1/a^2) and the electric field at the surface of the second sphere is E2 = k * (q2/b^2).
Step 3: Understanding the connection
- Since the two spheres are connected by a wire, they are at the same potential.
- This means that the electric potential at the surface of both spheres is the same.
- The electric potential at the surface of a sphere is given by the equation V = k * (q/r), where V is the electric potential, q is the charge on the sphere, and r is the radius of the sphere.
- Therefore, the electric potential at the surface of the first sphere is V1 = k * (q1/a) and the electric potential at the surface of the second sphere is V2 = k * (q2/b).
Step 4: Ratio of electric fields
- The electric field at a point is the negative gradient of the electric potential at that point.
- Therefore, the ratio of electric fields at the surfaces of the two spheres is given by the equation E1/E2 = (dV1/dr)/(dV2/dr).
- Since the potential is constant at the surface of a sphere, the derivative of the potential with respect to the radius is zero.
- Therefore, the ratio of electric fields at the surfaces of the two spheres is E1/E2 = 0/0, which is an indeterminate form.
Step 5: Applying L'Hopital's Rule
- To evaluate the indeterminate form, we can apply L'Hopital's Rule, which states that if the limit of the ratio of two functions is of the form 0/0 or infinity/infinity, then the limit of the ratio is equal to the limit of the ratio of the derivatives of the two functions.
- Applying L'Hopital's Rule to the ratio E1/E2, we have E1/E2 = (d^2V1/dr^2)/(d^2V2/dr^2).
Step 6: Derivatives of electric potentials
- Taking the derivatives of the electric potentials V1 and V2 with respect to the radius, we have dV1/dr = k * (dq1/dr)/a and dV2/dr = k * (dq2/dr)/b.
Step 7: Ratio of charge derivatives