Coulomb's Law: Exercises

Coulomb's law is used to calculate the magnitude of the electrical force between two charges.

This law says that the force intensity is equal to the product of a constant, called constant electrostatics, by the modulus of the value of the charges, divided by the square of the distance between the charges, i.e:

F equals numerator k. open vertical bar Q with 1 subscript closes vertical bar. open vertical bar Q with 2 subscript close vertical bar over denominator d squared end of fraction

Take advantage of the resolution of the questions below to clear your doubts regarding this electrostatic content.

Resolved issues

1) Fuvest - 2019

Three small spheres charged with a positive charge ܳ occupy the vertices of a triangle, as shown in the figure. In the inner part of the triangle is affixed another small sphere, with a negative charge q. The distances of this charge to the other three can be obtained from the figure.

Fuvest 2019 electric power issue

Where Q = 2 x 10-4 C, q = - 2 x 10-5 C and ݀d = 6 m, the net electric force on the charge q

(The constant k0 Coulomb's law is 9 x 109 No. m22)

a) is null.
b) has y-axis direction, downward direction and 1.8 N modulus.
c) has y-axis direction, upward direction and 1.0 N modulus.


d) has y-axis direction, downward direction and 1.0 N modulus.
e) has y-axis direction, upward direction and 0.3 N module.

To calculate the net force on the load q it is necessary to identify all the forces acting on this load. In the image below we represent these forces:

Fuvest issue 2019 Coulomb law

Charges q and Q1 are located at the vertex of the right triangle shown in the figure, which has legs measuring 6 m.

Thus, the distance between these charges can be found through the Pythagorean theorem. So we have:

d with 12 subscript equals 6 squared plus 6 squared d with 12 subscript equals 6 square root of 2 m

Now that we know the distances between the charges q and Q1, we can calculate the strength of the force F1 among them applying Coulomb's law:

F equals numerator k. open vertical bar Q with 1 subscript closes vertical bar. open vertical bar Q with 2 subscript close vertical bar over denominator d squared end of fraction
F with 1 subscript equal to numerator 9.10 to the power of 9. space 2.10 to the power of minus 4 end of the exponential. space 2.10 to the minus 5 end power of the exponential over denominator left parenthesis 6 square root of 2 right parenthesis squared end of fraction F with 1 subscript equal to 36 over 72 equal to 1 half space N

The strength of the F force2 between q and q charges2 will also be equal to 1 half N, because the distance and the value of the charges are the same.

To calculate the net force F12 we use the parallelogram rule, as shown below:

Fuvest Question 2019 Coulomb's Law
F with 12 subscript squared equals left parenthesis 1 half right parenthesis squared plus left parenthesis 1 half right parenthesis squared F with 12 subscript equal to square root of 2 over 4 end of root F with 12 subscript equal to numerator square root of 2 over denominator 2 end of fraction space N

To calculate the force value between q and Q loads3 we again apply Coulomb's law, where the distance between them is equal to 6 m. Thus:

F with 3 subscript equal to numerator 9.10 to the power of 9. space 2.10 to the power of minus 4 end of the exponential. space 2.10 to the power of minus 5 end of exponential over denominator 6 squared end of fraction F with 3 subscript equal to 36 over 36 equal to 1 N

Finally, we will calculate the net force on the charge q. Note that the F forces12 and F3 have the same direction and opposite direction, so the resulting force will be equal to the subtraction of these forces:

F with R subscript equal to 1 minus square root numerator of 2 over denominator 2 end of fraction F with R subscript equal to numerator 2 minus square root of 2 over denominator 2 end of fraction F with R subscript approximately equal 0 comma 3 N space

How F3 has a module greater than F12, the result will point up in the y-axis direction.

Alternative: e) has y-axis direction, upward direction and 0.3 N modulus.

To learn more, see Coulomb's Law and electric power.

2) UFRGS - 2017

Six electrical charges equal to Q are arranged, forming a regular hexagon with edge R, as shown in the figure below.

UFRGS Electric Power Issue 2017

Based on this arrangement, with k being the electrostatic constant, consider the following statements.

I - The resulting electric field in the center of the hexagon has a modulus equal to numerator 6 k Q over denominator R squared end of fraction
II - The work required to bring a charge q, from infinity to the center of the hexagon, is equal to numerator 6 k Q q over denominator R end of fraction
III - The resultant force on a test load q, placed in the center of the hexagon, is null.

Which ones are correct?

a) Only I.
b) Only II.
c) Only I and III.
d) Only II and III.
e) I, II and III.

I - The electric field vector in the center of the hexagon is null, as the vectors of each charge have the same modulus, they cancel each other out, as shown in the figure below:

UFRGS issue 2017 Coulomb law

So the first statement is false.

II - To calculate the work we use the following expression T = q. ΔU, where ΔU is equal to the potential at the center of the hexagon minus the potential at infinity.

Let's define the potential at infinity as null and the value of the potential at the center of the hexagon will be given by the sum of the potential relative to each charge, since the potential is a scalar quantity.

Since there are 6 charges, then the potential at the center of the hexagon will be equal to: U equals 6. numerator k Q over denominator d end of fraction. In this way, the work will be given by: T equal to numerator 6 k Q q over denominator d end of fraction, therefore, the statement is true.

III - To calculate the net force at the center of the hexagon, we do a vector sum. The resultant force value at the center of the hex will be zero. So the alternative is also true.

Alternative: d) Only II and III.

To learn more, see also Electric field and Electric Field Exercises.

3) PUC/RJ - 2018

Two electrical charges +Q and +4Q are fixed on the x-axis, respectively at positions x = 0.0 m and x = 1.0 m. A third charge is placed between the two, on the x-axis, such that it is in electrostatic equilibrium. What is the position of the third charge, in m?

a) 0.25
b) 0.33
c) 0.40
d) 0.50
e) 0.66

When placing a third load between the two fixed loads, regardless of its sign, we will have two forces of the same direction and opposite directions acting on this load, as shown in the figure below:

Question Puc/RJ 2018 Coulomb Law

In the figure, we assume that charge Q3 is negative and since the charge is in electrostatic equilibrium, then the net force is equal to zero, like this:

F with 13 subscript equal to numerator k. Q. q over denominator x squared end of fraction F with 23 subscript equal to numerator k. q.4 Q over denominator left parenthesis 1 minus x right parenthesis squared end of fraction F with R subscript space end of subscript equal to space F with 13 subscript minus F with 23 subscript equal to 0 diagonal numerator upward risk k. diagonal up risk q. diagonal up risk Q over denominator x squared end of fraction equals numerator diagonal up risk k. diagonal up risk q.4 diagonal up risk Q over denominator left parenthesis 1 minus x right parenthesis squared end of fraction 4 x squared equals 1 minus 2 x plus x squared 4x squared minus x squared plus 2x minus 1 equals 0 3x squared plus 2x minus 1 equals 0 increment equals 4 minus 4.3. left parenthesis minus 1 parenthesis right increment equal to 4 plus 12 equal to 16 x equal to numerator minus 2 plus or minus square root of 16 over denominator 2.3 end of fraction x with 1 subscript equal to numerator minus 2 plus 4 over denominator 6 end of fraction equal to 1 third approximately equal 0 point 33 x with 2 subscript equal to numerator minus 2 minus 4 over denominator 6 end of fraction equal to numerator minus 6 over denominator 6 end of fraction equals minus 1 space left parenthesis e st e space p o n t o space n o space e s t á space e n t r e space a s space c a r g a s right parenthesis

Alternative: b) 0.33

To learn more, see electrostatics and Electrostatics: Exercises.

4) PUC/RJ - 2018

A load that0 is placed in a fixed position. When placing a load q1 =2q0 at a distance d from q0, what1 suffers a repulsive force of modulus F. Replacing q1 for a load that2 in the same position, which2 suffers an attractive force of 2F modulus. If the loads q1 and what2 are placed at a 2d distance from each other, the force between them is

a) repulsive, of module F
b) repulsive, with a 2F module
c) attractive, with module F
d) attractive, with 2F module
e) attractive, 4F module

As the force between the charges qO and what1 is repulsion and between charges qO and what2 is of attraction, we conclude that the loads q1 and what2 have opposite signs. In this way, the force between these two charges will be of attraction.

To find the magnitude of this force, we will start by applying Coulomb's law in the first situation, that is:

F equals numerator k. q with 0 subscript. q with 1 subscript over denominator d squared end of fraction

Being the load q1 = 2 q0the previous expression will be:

F equals numerator k. q with 0 subscript.2 q with 0 subscript over denominator d squared end of fraction equal to numerator 2. k. q with 0 squared subscript over denominator d squared end of fraction

When replacing q1 why2 the force will be equal to:

2 F equals numerator k. q with 0 subscript. q with 2 subscript over denominator d squared end of fraction

Let's isolate the charge that2 on a two sides of the equality and replace the value of F, so we have:

q with 2 subscript equal to 2 F. numerator d squared over denominator k. q with 0 subscript end of fraction q with 2 subscript equal to 2. numerator 2. diagonal up risk k. strike out diagonally up over q with 0 subscript end of strikeout squared over denominator strike out diagonally up over d squared end of strikeout end of fraction. numerator crossed out diagonally up over d squared end of crossed out over denominator diagonally up risk k. diagonal strike up over q with 0 subscript end of strikeout end of fraction equal to 4. q with 0 subscript

To find the net force between the charges q1 and what2, let's apply Coulomb's law again:

F with 12 subscript equal to numerator k. q with 1 subscript. q with 2 subscript over denominator d with 12 subscript squared end of fraction

Replacing q1 for 2q0, what2 by 4q0 and of12 by 2d, the previous expression will be:

F with 12 subscript equal to numerator k.2 q with 0 subscript.4 q with 0 subscript over denominator left parenthesis 2 d right parenthesis squared end of fraction equals diagonal numerator up risk 4.2 k. q with 0 squared subscript over diagonal denominator upwards risk 4 d squared end of fraction

Observing this expression, we notice that the module of F12 = F.

Alternative: c) attractive, with module F

5) PUC/SP - 2019

A spherical particle electrified with a charge of modulus equal to q, of mass m, when placed on a flat, horizontal, perfectly smooth surface with its center a a distance d from the center of another electrified particle, fixed and also with a charge of modulus equal to q, is attracted by the action of the electric force, acquiring an acceleration α. It is known that the electrostatic constant of the medium is K and the magnitude of the acceleration of gravity is g.

Determine the new distance d’, between the centers of the particles, on this same surface, however, with it now inclined at an angle θ, in relation to the horizontal plane, so that the load system remains in balance static:

Electric power issue Puc-SP 2019
right parenthesis space d ´ equals numerator P. s and n theta. k. q squared over denominator left parenthesis A minus right parenthesis end of fraction b right parenthesis space d ´ equal to numerator k. q squared over denominator P left parenthesis A minus right parenthesis end of fraction c right parenthesis space d ´ equals numerator P. k. q squared over denominator left parenthesis A minus right parenthesis end of fraction d right parenthesis space d ´ equal to numerator k. q squared. left parenthesis A minus right parenthesis on denominator P. s and n theta end of fraction

For the load to remain in equilibrium on the inclined plane, the component of the force weight must be in the direction tangent to the surface (Pt ) is balanced by electrical force.

In the figure below we represent all the forces acting on the load:

Question PUC/SP 2018 Coulomb Law

The P componentt of the weight force is given by the expression:

Pt = P. if not

The sine of an angle is equal to the division of the measure of the opposite leg by the measure of the hypotenuse, in the image below we identify these measures:

Puc/sp question 2018 Coulomb law

From the figure, we conclude that sen θ will be given by:

s and n space theta equal to numerator left parenthesis Minus right parenthesis on denominator d ´ end of fraction

Substituting this value in the weight component expression, we are left with:

P with t subscript equal to P. numerator space left parenthesis Minus right parenthesis on denominator ´ end of fraction

As this force is being balanced by the electrical force, we have the following equality:

P. numerator left parenthesis A minus right parenthesis over denominator d ` end of fraction equals numerator k. q squared over denominator d ´ squared end of fraction

Simplifying the expression and isolating the d', we have:

P. numerator left parenthesis A minus right parenthesis over denominator slashed diagonally up over d ´ end of strikeout end of fraction equals numerator k. q squared over denominator slashed diagonally up over d ´ squared end of strikeout end of fraction d ´ equal to numerator k. q squared over denominator P. left parenthesis Unless right parenthesis end of fraction

Alternative: b right parenthesis space d ´ equal to numerator k. q squared over denominator P. left parenthesis Unless right parenthesis end of fraction

6) UERJ - 2018

The diagram below represents the metallic spheres A and B, both with masses of 10-3 kg and electrical load of module equal to 10-6 Ç. The spheres are attached by insulating wires to supports, and the distance between them is 1 m.

UERJ 2018 issue Coulomb law

Assume that the wire holding sphere A has been cut and that the net force on that sphere corresponds only to the electrical interaction force. Calculate the acceleration, in m/s2, acquired by ball A immediately after cutting the wire.

To calculate the value of the acceleration of the sphere after cutting the wire, we can use Newton's 2nd law, ie:

FR = m. The

Applying Coulomb's law and equating the electric force to the resulting force, we have:

numerator k. open vertical bar Q with A subscript close vertical bar. open vertical bar Q with subscript B close vertical bar over denominator d squared end of fraction equal to m. The

Replacing the values ​​indicated in the problem:

numerator 9.10 to the power of 9.10 to the power of minus 6 end of the exponential.10 to the power of minus 6 end of the exponential over denominator 1 squared end of fraction equal to 10 to the power of minus 3 end of exponential. The
a equal to numerator 9.10 to the minus 3 end of the exponential over denominator 10 to the minus 3 end of the exponential end of the fraction a equal to 9 m space divided by s squared

7) Unicamp - 2014

The attraction and repulsion between charged particles has numerous industrial applications, such as electrostatic painting. The figures below show the same set of charged particles, at the vertices of a square side a, that exert electrostatic forces on charge A at the center of this square. In the situation presented, the vector that best represents the net force acting on load A is shown in figure

Unicamp 2014 issue electric power

The force between charges of the same sign is attraction and between charges of opposite signs is repulsion. In the image below we represent these forces:

Unicamp issue 2014 Coulomb law

Alternative: d)

Coulomb's Law: formula, graph, examples and exercises

Coulomb's Law: formula, graph, examples and exercises

 THE lawinCoulomb is an important law of physics that states that the electrostatic force between...

read more
5 things you need to know about waves

5 things you need to know about waves

THE undulatory is the branch of Physics which studies all the phenomena related to the different ...

read more
Light absorption: what it is and its relationship to colors

Light absorption: what it is and its relationship to colors

THE absorptiongiveslight is a process by which the light that focuses on a body is converted into...

read more