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Jet001 [13]
2 years ago
15

Two identical conducting spheres, fixed in place, attract each other with an electrostatic force of -0.2589 N when separated by

50 cm, center-to-center. The spheres are then connected by a thin conducting wire. When the wire is removed, the spheres repel each other with an electrostatic force of 0.3456 N. What were the initial charges on the spheres? Since one is negative and you cannot tell which is positive or negative, there are two solutions. Take the absolute value of the charges and enter the smaller value here. Enter the larger value here.
Physics
1 answer:
Harlamova29_29 [7]2 years ago
3 0

Answer:

q_1 = 7.19 \times 10^{-6} C

q_2 = -1.0 \times 10^{-6} C

Explanation:

Let the initial charge on the two spheres are

q_1, -q_2

now we know that the force between them is given as

F = \frac{kq_1q_2}{r^2}

0.2589 = \frac{kq_1q_2}{0.5^2}

q_1q_2 = 7.19 \times 10^{-12}

now when two spheres are connected then final charge on them is given as

q = \frac{q_1 - q_2}{2}

now the force between them is given as

0.3456 = \frac{k(q_1 - q_2)^2}{4(0.5)^2}

now we have

q_1 - q_2 = 6.19 \times 10^{-6}

So by solving above two equations we have

q_1 = 7.19 \times 10^{-6} C

q_2 = -1.0 \times 10^{-6} C

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2 years ago
A block–spring system vibrating on a frictionless, horizontal surface with an amplitude of 7.0 cm has an energy of 14 J. If the
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Answer:

E_T= 28J

Explanation:

The energy of Mass-Spring System the sum of the potential energy of the block plus the kinetic energy of the block:

E_T=U+K=\frac{1}{2} k \Delta x^2+\frac{1}{2} mv^2

Where:

\Delta x=Amplitude\hspace{3}or\hspace{3}d eformation\hspace{3} of\hspace{3} the\hspace{3} spring\\m=Mass\hspace{3}of\hspace{3}the\hspace{3}block\\k=Constant\hspace{3}of\hspace{3}the\hspace{3}spring\\v=Velocity\hspace{3}of\hspace{3}the\hspace{3}block

There are two cases, the first case is when the spring is compressed to its maximum value, in this case the value of the kinetic energy is zero, since there is no speed, so:

E_T=\frac{1}{2} k \Delta x^2\\\\14=\frac{1}{2} k7^2\\\\Solving\hspace{3} for\hspace{3} k\\\\k=\frac{28}{49} =\frac{4}{7}

The second case is when the block passes through its equilibrium position, in this case the elastic potential energy is zero since \Delta x=0, so:

E_T=\frac{1}{2} mv^2\\\\14=\frac{1}{2} mv^2\\\\Solving\hspace{3} for\hspace{3} v\\\\v^2=\frac{28}{m}

Now, let's find the energy of the system when the block is replaced by one whose mass is twice the mass of the original block using the previous data:

E_T=U+K=\frac{1}{2} k \Delta x^2+\frac{1}{2} m_2v^2

Where in this case:

m_2=New\hspace{3}mass=Twice\hspace{3} the\hspace{3} mass \hspace{3}of\hspace{3} the\hspace{3} original=2m

Therefore:

E_T=\frac{1}{2} (\frac{4}{7} ) (7^2)+\frac{1}{2} (2m)(\frac{28}{m_2})=\frac{1}{2} (\frac{4}{7} ) (7^2)+\frac{1}{2} (2m)(\frac{28}{2m})=14+14=28J

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