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Coulombs Law and Electric Field Questions and Answers

Answer: A

The force is \( F = Q_1 Q_2/(4\pi\epsilon_0 R^2) \), directed along the line joining the charges and repulsive for like signs. The inverse square dependence is what makes Gauss's law take so simple a form in three dimensions.

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Answer: B

Correct answer: \( 9 \times 10^{9} \)

With \( \epsilon_0 = 8.85\times10^{-12} \) F/m, \[ \frac{1}{4\pi\epsilon_0} = 8.99\times10^{9} \approx 9\times10^{9}\ \mathrm{N\,m^2\,C^{-2}}. \] The 8.85 offered is the permittivity itself rather than the constant built from it, \( 3\times10^{8} \) is the speed of light, and \( 4\pi\times10^{-7} \) is the permeability of free space.

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Answer: D

Coulomb's law gives a positive product for like charges and the vector form then points each charge away from the other. The force acts along the line of centres, which is what makes it a central force and conserves angular momentum about either charge.

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Answer: A

Superposition holds because Maxwell's equations are linear, so each source contributes independently. The vector nature matters: two equal and opposite contributions cancel entirely, which is how a field-free point arises between two like charges.

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6.

Doubling the separation of two point charges changes the force between them to

Answer: B

Correct answer: a quarter of its former value

Coulomb’s law goes as the inverse square, \( F \propto 1/r^2 \), so doubling the separation divides the force by \( 2^2 = 4 \). The eighth offered would apply to an inverse cube, which is the dipole field rather than the point charge force - a distinction the dipole item in this topic makes explicitly.

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Answer: C

Writing \( \mathbf{E} = \mathbf{F}/Q \) removes the test charge from the description and leaves a property of the source alone. The work per unit charge from infinity is the potential, which is a different and scalar quantity.

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9.

The electric field at a distance \( R \) from a point charge \( Q \) has magnitude

Answer: A

Dividing Coulomb's force by the test charge leaves this expression, directed radially outward for a positive charge. The three wrong answers are each a correct formula for something else, which is why keeping the geometry in mind matters more than memorising forms.

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10.

The field of an infinite straight line charge of density \( \rho_L \) at a distance \( \rho \) is

Answer: B

Applying Gauss's law to a cylinder round the line gives an area proportional to the radius, so the field falls as the first power rather than the square. It points radially away from the line and has no component along it.

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