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Question: Eight tiny drops are combined to form a big drop. If the potential on each drop is 10 V then potenti...

Eight tiny drops are combined to form a big drop. If the potential on each drop is 10 V then potential of big drop will be-
A. 40V
B. 10V
C. 30V
D. 20V

Explanation

Solution

To solve this problem first we need to find the radius of the new big drop, which can be calculated by equating the total volume of 8 drops to the final big drop. Now to calculate potential we need to calculate total charge on the big drop than by applying formula we can calculate potential on big drop.

Formula used:
V=kqrV=\dfrac{kq}{r}
And, volume of sphere=43πr3\dfrac{4}{3}\pi {{r}^{3}}

Complete Step by step solution:

Given, potential on each drop = 10V

Now, by combining each drop the volume of resultant drop will be equal to 8 times of volume of small drop so,
8×Vs=VL8\times {{V}_{s}}={{V}_{L}} , here Vs{{V}_{s}}(volume of small drops) and VL{{V}_{L}}(volume of large drop)

Now, 8×43πr3=43πR38\times \dfrac{4}{3}\pi {{r}^{3}}=\dfrac{4}{3}\pi {{R}^{3}}
R=2r\Rightarrow R=2r …....(1)
R (radius of big drop) and r (radius of small drop)

Now, Potential V=kqrV=\dfrac{kq}{r}, here k (constant = 14πε0\dfrac{1}{4\pi\varepsilon_{0}}), q (charge on sphere) and r(radius of sphere)
If small drops having a charge of q than big drop will be having a charge of Q=8q, because total charge will be conserve,

Now for small drops potential V=kqrV=\dfrac{kq}{r} ………(2)

For big drop potential V=kQRV=\dfrac{kQ}{R} …… (3)

From equation (1), (2) and (3) we have,
bigdroppotentialV=kQR=k×8q2r\Rightarrow big drop potential V=\dfrac{kQ}{R}=\dfrac{k\times 8q}{2r}
4k×qr\Rightarrow 4\dfrac{k\times q}{r}=4(potential of small drop from equation 2)
4×10=40V\Rightarrow 4\times 10=40V

So, the potential of a big drop will be 40V, hence option (A) will be correct.

Note:
While solving these type of problem conservation of charge and volume should be kept in mind as the total charge and volume will be equal to sum of all small spheres and this rule is not restricted only for spheres for any shape and size these two will be conserved but the difficult part would be to derive formula for potential and volume for those irregular shapes