Answer:
Step-by-step explanation:
Part A:
Using the formula for electric potential due to a charged spherical shell:
V1 = kq1/R1 and V2 = kq2/R2
where k is the Coulomb constant.
For r < R1, the electric potential due to both shells is:
V = V1 + V2 = kq1/R1 + kq2/R2
For R1 < r < R2, the electric potential due to the outer shell is:
V = V2 = kq2/R2
For r > R2, the electric potential due to both shells is:
V = V1 + V2 = kq1/r + kq2/R2
Substituting the given values, we get:
V = (9.0x10^9 Nm^2/C^2)(5.00x10^-6 C)/0.025 m + (9.0x10^9 Nm^2/C^2)(-6.00x10^-6 C)/0.15 m
V = -4.32x10^5 V
Therefore, the electric potential due to the two shells at a distance of 2.50 cm from their common center is -4.32x10^5 V.
Part B:
For r < R1, the electric potential due to both shells is:
V = V1 + V2 = kq1/R1 + kq2/R2
For R1 < r < R2, the electric potential due to both shells is:
V = V1 + V2 = kq1/r + kq2/R2
For r > R2, the electric potential due to both shells is:
V = V1 + V2 = kq1/r + kq2/r
Substituting the given values, we get:
V = (9.0x10^9 Nm^2/C^2)(5.00x10^-6 C)/0.1 m + (9.0x10^9 Nm^2/C^2)(-6.00x10^-6 C)/0.1 m
V = 4.80x10^5 V
Therefore, the electric potential due to the two shells at a distance of 10.0 cm from their common center is 4.80x10^5 V.