Question #55540

For a single, isolated point charge carrying a charge of q = 5.77 × 10-11 C, one equipotential surface consists of a sphere of radius 0.0329 m centered on the point charge as shown. What is the potential on this surface?

Answer in V=

You would like to draw an additional equipotential surface, which is separated by 4.90 V from the previously mentioned surface. How far from the point charge should this surface be? This surface must also meet the condition of being farther from the point charge than the original equipotential surface.

Answer in m=
1

Expert's answer

2015-10-17T09:54:26-0400

Answer on Question#55540 - Physics - Electromagnetism

For a single, isolated point charge carrying a charge of q=5.77×1011Cq = 5.77 \times 10^{-11} \mathrm{C}, one equipotential surface consists of a sphere of radius r=0.0329mr = 0.0329 \mathrm{m} centered on the point charge as shown. What is the potential on this surface?

Answer in V=V =

You would like to draw an additional equipotential surface, which is separated by Δφ=4.90V\Delta \varphi = 4.90\mathrm{V} from the previously mentioned surface. How far from the point charge should this surface be? This surface must also meet the condition of being farther from the point charge than the original equipotential surface.

Answer in m=m =

**Solution:**

The potential φ\varphi at distance rr from the charge qq is given by


φ=keqr,\varphi = \frac {k _ {e} q}{r},


where ke=8.98755×109Nm2C2k_{e} = 8.98755 \times 10^{9} \frac{\mathrm{N} \cdot \mathrm{m}^{2}}{\mathrm{C}^{2}} – is Coulomb's constant. Therefore at distance r=0.0329mr = 0.0329 \, \mathrm{m} the potential is


φ1=8.98755×109Nm2C25.77×1011C0.0329m=15.76V\varphi_ {1} = \frac {8.98755 \times 10 ^ {9} \frac {\mathrm {N} \cdot \mathrm {m} ^ {2}}{\mathrm {C} ^ {2}} \cdot 5.77 \times 10 ^ {- 1 1} \mathrm {C}}{0.0329 \, \mathrm {m}} = 15.76 \mathrm {V}


The potential difference between φ1\varphi_{1} and φ2\varphi_{2} (the potential of the equipotential surface whose radius r2r_{2} we want to find) is given by


Δφ=φ1φ2=φ1keqr2\Delta \varphi = \varphi_ {1} - \varphi_ {2} = \varphi_ {1} - \frac {k _ {e} q}{r _ {2}}


Therefore the radius r2r_2 is


r2=keqφ1Δφ=8.98755×109Nm2C25.77×1011C15.76V4.90V=0.0478mr _ {2} = \frac {k _ {e} q}{\varphi_ {1} - \Delta \varphi} = \frac {8.98755 \times 10 ^ {9} \frac {\mathrm {N} \cdot \mathrm {m} ^ {2}}{\mathrm {C} ^ {2}} \cdot 5.77 \times 10 ^ {- 1 1} \mathrm {C}}{15.76 \mathrm {V} - 4.90 \mathrm {V}} = 0.0478 \mathrm {m}


**Answer:** 15.76V, 0.0478m.

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