Exercises on potential and kinetic energy

Study about kinetic and potential energy with this list of solved exercises that Toda Matter has prepared for you. He solves his doubts with step-by-step resolutions and prepares himself with ENEM and entrance exam questions.

question 1

In a market, two workers are loading a truck that will deliver vegetables. The operation takes place as follows: worker 1 removes the vegetables from a stall and keeps them in a wooden box. Afterwards, he throws the box, making it slide on the ground, towards worker 2 who is beside the truck, in charge of storing it on the body.

Worker 1 throws the box with an initial speed of 2 m/s and the friction force performs a modulus job equal to -12 J. The wooden box plus vegetables set has a mass of 8 kg.
Under these conditions, it is correct to state that the speed at which the box reaches worker 2 is

a) 0.5 m/s.
b) 1 m/s.
c) 1.5 m/s.
d) 2 m/s.
e) 2.5 m/s.

Correct answer: b) 1 m/s

The work of the forces acting on a body is equal to the change in the energy of that body. In this case, kinetic energy.

tau equals increment E with subscript c

The change in kinetic energy is the final kinetic energy minus the initial kinetic energy.

tau equal to increment E with C with f subscript end of subscript minus increment E with C with i subscript end of subscript tau equal to numerator m. v with f squared subscript over denominator 2 end of fraction minus numerator m. v with i squared subscript over denominator 2 end of fraction

From the statement, we have that the work is - 16 J.

The speed at which the box reaches worker 2 is the final speed.

minus 12 equals numerator 8. v with f squared subscript over denominator 2 end of fraction minus numerator 8.2 squared over denominator 2 end of fraction

Solving for Vf

minus 12 equals 8 over 2 open parenthesis v with f squared subscript minus 4 close parenthesis minus 12 equals 4 open parenthesis v with f squared subscript minus 4 close parentheses numerator minus 12 over denominator 4 end of fraction equal to open parenthesis v with f subscript squared minus 4 close parenthesis minus 3 equal to v with f subscript to square minus 4 minus 3 plus 4 equal to v with f subscript squared 1 equal to v with f subscript squared square root of 1 equal to v with f subscript 1 space m divided by s equal a v with f subscript

Therefore, the speed at which the box reaches worker 2 is 1 m/s.

question 2

In a bagged grain warehouse, a large shelf with four shelves 1.5 m high stores the goods that will be shipped. Still on the ground, six sacks of grain weighing 20 kg each are placed on a wooden pallet, which is collected by a forklift. Each pallet has 5 kg of mass.

Considering the acceleration of gravity equal to 10 m/s², the set bags plus pallet as a body and disregarding its dimensions, the energy gravitational potential acquired by the pallet set plus bags of grain, as they leave the ground and are stored on the fourth floor of the shelf, stands for

a) 5400 J.
b) 4300 J.
c) 5 625 J.
d) 7200 J.
e) 7,500 J.

Correct answer: c) 5 625 J

The gravitational potential energy of a body is the product of the mass of that body, the magnitude of the acceleration due to gravity and its height in relation to the ground.

And with p subscript equal to m. g. H

Calculation of mass

As each bag of grain has 20 kg of mass and the pallet is 5 kg, the set has:

20.6 + 5 = 120 + 5 = 125 kg

The height

The bookcase has 4 floors of 1.5 m and the set will be stored on the fourth. Its height will be 4.5 m from the ground, as shown in the drawing. Note that the set is not on the fourth floor but on the fourth floor.

Thus:

And with p subscript equal to m. g. h E with p subscript equal to 125.10.4 point 5 E with p subscript equal to 5 space 625 space J

The energy acquired by the set will be 5 625 J.

question 3

A spring that has a length of 8 cm when at rest receives a compressive load. An 80 g mass body is placed over the spring and its length is reduced to 5 cm. Considering the acceleration of gravity as 10 m/s² determine:

a) The force acting on the spring.
b) The elastic constant of the spring.
c) The potential energy stored by the spring.

a) The force acting on the spring corresponds to the weight force exerted by the 80 g mass.

The force weight is obtained by the product of mass and the acceleration due to gravity. It is necessary that the mass is written in kilograms.

80 g = 0.080 kg.

P equals m g P equals 0 comma 080.10 P equals 0 comma 80 space N

The force acting on the spring is 0.80 N.

b) In the vertical direction, only the weight force and the elastic force act, in opposite directions. Once static, the elastic force cancels out with the weight force, having the same modulus.

The deformation x was 8 cm - 5 cm = 3 cm.

The relationship that provides the tensile strength is

F with e l subscript end of subscript equal to k. x where k is the elastic constant of the spring.

k equal to F with e l subscript end of subscript over x k equal to numerator 0 comma 80 over denominator 3 end of fraction k approximately equal 0 comma 26 space N divided by c m

c) The potential energy stored in a spring is given by the equation of work of elastic force.

tau with F with e l subscript end of subscript end of subscript equal to numerator k. x squared over denominator 2 end of fraction

Replacing the values ​​in the formula and calculating, we have:

tau with F with e l subscript end of subscript subscript end of subscript equal to numerator 0 comma 26. left parenthesis 0 comma 03 right parenthesis squared over denominator 2 end of fraction tau with F with and l subscript end of subscript subscript end of subscript equal to numerator 0 comma 26.0 comma 0009 over denominator 2 end of fraction tau with F with and l subscript end of subscript subscript end of subscript equal to numerator 0 comma 000234 over denominator 2 end of fraction tau with F with and 1 subscript end of subscript end of subscript equal to 0 comma 000117 J space

in scientific notation 1 comma 17 multiplication sign 10 to the minus 4 power end of exponential space J

question 4

A body with a mass equal to 3 kg is free-falling from a height of 60 m. Determine the mechanical, kinetic and potential energy at times t = 0 and t = 1s. Consider g = 10 m/s².

Mechanical energy is the sum of kinetic and potential energy at each instant.

E with M subscript equals E with P subscript plus E with C subscript

Let's calculate the energies for t = 0s.

Kinetic energy at t = 0s.

At t=0s the speed of the body is also zero, as the body is abandoned, leaving rest, so the kinetic energy is equal to 0 Joules.

And with C subscript equal to numerator m. v squared over denominator 2 end of fraction E with C subscript equal to numerator 3.0 squared over denominator 2 end of fraction equal to 0 space J

Potential energy at t = 0s.

And with P subscript equal to m. g. h E with subscript P equal to 3.10.60 equal to 1800 J space

Mechanical energy at t = 0s.

And with M subscript equal to 1 space 800 plus 0 space equal to space 1 space 800 space J

Let's calculate the energies for t = 1s.

Kinetic energy at t = 1s.

First, it is necessary to know the velocity at t=1s.

For this, we will use the hourly velocity function for a MUV (uniformly varied movement).

V left parenthesis t right parenthesis equals V with 0 subscript plus a. t

Where,
V with 0 subscript space end of subscriptis the initial speed,
The is the acceleration, which in this case will be the acceleration of gravity, g,
t is the time in seconds.

The initial movement speed is 0, as we've already seen. The equation looks like this:

V left parenthesis t right parenthesis equal to g. t

Using g = 10 and t = 1,

V left parenthesis 1 right parenthesis equal to 10.1 V left parenthesis 1 right parenthesis equal to 10 m space divided by s

Which means that in 1s of fall the velocity is 10 m/s and now we can calculate the kinetic energy.

And with C subscript equal to numerator m. v squared over denominator 2 end of fraction E with C subscript equals numerator 3.10 squared over denominator 2 end of fraction E with C subscript equal to numerator 3,100 over denominator 2 end of fraction equal to numerator 3,100 over denominator 2 end of fraction equal to 300 over 2 equal to 150 space J

Potential energy for t=1s.

To know the potential energy at t=1s, we first need to know how high it is at this instant. In other words, how far it has shifted. For that, we will use the hourly function of the positions for t=1s.

Where, S with 0 subscript is the starting position of the move, which we will consider as 0.

S equals S with 0 subscript plus V with 0 subscript. t more g over 2. t squared S equals 0 plus 0. t plus 10 over 2.1 squared S equals 10 over 2.1 equals 5 m space

Therefore, at t=1s the body will have traveled 5 m and its height in relation to the ground will be:

60 m - 5 m = 55 m

Now we can calculate the potential energy for t=1s.

And with P subscript equal to m. g. h E with P subscript equal to 3.10.55 space equal to space 1 space 650 space J.

Calculating mechanical energy for t=1s.

E with M subscript equal to E with P subscript plus E with C subscript E with M subscript equal to 1 space 650 plus 150 space equal to space 1 space 800 space J

See that the mechanical energy is the same, I try for t = 0s as for t = 1s. As the potential energy decreased, the kinetics increased, compensating for the loss, as it is a conservative system.

question 5

A child is playing on a swing in a park with his father. At a certain point, the father pulls the swing, raising it to a height of 1.5 m in relation to where it is at rest. The swing set plus child has a mass equal to 35 kg. Determine the horizontal speed of the swing as it passes through the lowest part of the trajectory.

Consider a conservative system where there is no energy loss and the acceleration due to gravity is equal to 10 m/s².

All potential energy will transform into kinetic energy. In the first moment the potential energy is

And with P subscript equal to m. g. h E with subscript P equal to 35.10.1 point 5 equal to 525 space J

In the second instant the kinetic energy will be equal to 525 J because all potential energy becomes kinetic.

And with C subscript equal to numerator m. v squared over denominator 2 end of fraction 525 equals numerator 35. v squared over denominator 2 end of fraction 525.2 equals 35. v squared 1050 over 35 equals v squared 30 equals v squared square root of 30 equals v space

Therefore, the horizontal velocity of the body is square root of 30 end space of root m divided by s space, or approximately 5.47 m/s.

question 6

(Enem 2019) At a science fair, a student will use the Maxwell disk (yo-yo) to demonstrate the principle of energy conservation. The presentation will consist of two steps:

Step 1 - the explanation that, as the disk descends, part of its gravitational potential energy is transformed into kinetic energy of translation and kinetic energy of rotation;

Step 2 - the calculation of the kinetic energy of rotation of the disk at the lowest point of its trajectory, assuming the conservative system.

When preparing the second step, he considers the acceleration due to gravity equal to 10 m/s² and the linear velocity of the center of mass of the disk negligible compared to the angular velocity. It then measures the height of the top of the disc relative to the ground at the lowest point of its trajectory, taking 1/3 of the height of the toy's shank.

The toy's size specifications, that is, of length (L), width (L) and height (H), as well as from the mass of its metal disk, were found by the student in the clipping of the illustrated manual to follow.

Contents: metal base, metal rods, top bar, metal disc.
Size (L × W × H): 300mm × 100mm × 410mm
Metal disk mass: 30 g

The result of the calculation of step 2, in joule, is:

right parenthesis space 4 comma 10 space multiplication sign space 10 to the minus power 2 end of exponential space b right parenthesis space 8 comma 20 space multiplication sign space 10 to the minus 2 end power of the exponential c right parenthesis space 1 comma 23 space multiplication sign space 10 to the minus 1 end power of the exponential space d right parenthesis space 8 comma 20 space multiplication sign space 10 to the power of 4 space end of exponential and right parenthesis space 1 comma 23 space multiplication sign space 10 to power of 5

Correct answer: b) And with C space d e space rotation subscript end of subscript equal to 8 comma 3 multiplication sign 10 to minus 2 end power of exponential J

We want to determine the kinetic energy of rotation at time 2, when the disk is at its lowest position.

Since the translation energy has been neglected, and there are no energy losses, all gravitational potential energy is transformed into kinetic energy of rotation.

Kinetic energy of rotation at the lowest point of the trajectory = Potential gravitational energy at the highest point of the trajectory.

The total height of the set is 410 mm or 0.41 m. The height of the trajectory is numerator 2 h over denominator 3 end of fraction it's the same as:

numerator 2 multiplication sign 0 comma 41 over denominator 3 end of fraction equal to numerator 0 comma 82 over denominator 3 end of fraction m

The mass is 30 g, in kilograms, 0.03 kg.

Calculating potential energy.

And with P subscript equal to m. g. h E with P subscript equal to 0 comma 03.10. numerator 0 comma 82 over denominator 3 end of fraction E with subscript P equal to 0 comma 3. numerator 0 comma 82 over denominator 3 end of fraction E with P subscript equal to 0 comma 1 space. space 0 comma 82 equals 0 comma 082 space J

In scientific notation, we have

And with C space d e space rotation subscript end of subscript equal to 8 comma 2 multiplication sign 10 to minus 2 end power of exponential J

question 7

(CBM-SC 2018) Kinetic energy is energy due to motion. Everything that moves has kinetic energy. Therefore, moving bodies have energy and therefore can cause deformations. The kinetic energy of a body depends on its mass and speed. Therefore, we can say that kinetic energy is a function of the mass and velocity of a body, where kinetic energy is equal to half its mass times its velocity squared. If we do some calculations, we will find that velocity determines a much greater increase in kinetic energy than mass, so we can conclude that there will be much greater injuries to occupants of a vehicle involved in a high-speed crash than to those in a low-speed crash velocity.

It is known that two cars, both weighing 1500 kg, collide in the same barrier. Car A has a speed of 20 m/s and vehicle B a speed of 35 m/s. Which vehicle will be more susceptible to a more violent collision and why?

a) Vehicle A, as it has a higher speed than vehicle B.
b) Vehicle B, as it has a constant speed higher than that of vehicle A.
c) Vehicle A, as it has the same mass as vehicle B, however it has a constant speed higher than vehicle B.
d) Both vehicles will be impacted with the same intensities.


Correct answer: b) Vehicle B, as it has a constant speed higher than vehicle A.

As the statement says, kinetic energy increases with the square of velocity, so a higher velocity produces greater kinetic energy.

By way of comparison, even if it is not necessary to answer the problem, let's calculate the energies of two cars and compare them.

car A

And with C A subscript end of subscript equal to numerator m. v squared over denominator 2 end of fraction space equals space numerator 1500.20 squared over denominator 2 end of fraction equal to numerator 1500.400 over denominator 2 end of fraction equal to 300 space 000 J space

car B

And with C A subscript end of subscript equal to numerator m. v squared over denominator 2 end of fraction space equals space numerator 1500.35 squared over denominator 2 end of fraction equal to numerator 1500.1225 over denominator 2 end of fraction equal to 918 space 750 J space

Thus, we see that the increase in the speed of car B leads to a kinetic energy more than three times greater than that of car A.

question 8

(Enem 2005) Observe the situation described in the strip below.

As soon as the boy shoots the arrow, there is a transformation from one type of energy to another. The transformation, in this case, is of energy

a) elastic potential in gravitational energy.
b) gravitational into potential energy.
c) elastic potential in kinetic energy.
d) kinetics in elastic potential energy.
e) gravitational into kinetic energy

Correct answer: c) elastic potential in kinetic energy.

1 - The archer stores energy in the elastic potential form, by deforming the bow that will act as a spring.

2 - When releasing the arrow, the potential energy is transformed into kinetic energy, when it goes into motion.

question 9

(Enem 2012) A car, in uniform motion, walks along a flat road, when it starts to descend a slope, on which the driver makes the car always keep up with climbing speed constant.

During the descent, what happens to the potential, kinetic, and mechanical energies of the car?

a) The mechanical energy remains constant, since the scalar velocity does not vary and, therefore, the kinetic energy is constant.
b) The kinetic energy increases, as the gravitational potential energy decreases and when one decreases, the other increases.
c) The gravitational potential energy remains constant, as there are only conservative forces acting on the car.
d) Mechanical energy decreases, as kinetic energy remains constant, but gravitational potential energy decreases.
e) The kinetic energy remains constant as there is no work done on the car.

Correct answer: d) Mechanical energy decreases as kinetic energy remains constant but gravitational potential energy decreases.

Kinetic energy depends on mass and velocity, as they do not change, kinetic energy remains constant.

The potential energy decreases as it depends on the height.

Mechanical energy decreases as this is the sum of potential energy plus kinetic energy.

question 10

(FUVEST 2016) Helena, whose mass is 50 kg, practices extreme sport bungee jumping. In a workout, it comes loose from the edge of a viaduct, with zero initial velocity, attached to an elastic band of natural length L with 0 subscript equal to 15 m space and elastic constant k = 250 N/m. When the swath is stretched 10 m beyond its natural length, Helena's modulus of velocity is

Note and adopt: gravity acceleration: 10 m/s². The band is perfectly elastic; its mass and dissipative effects should be ignored.

a) 0 m/s
b) 5 m/s
c) 10 m/s
d) 15 m/s
e) 20 m/s

Correct answer: a) 0 m/s.

By energy conservation, the mechanical energy at the start of the jump is equal at the end of the jump.

E with M i n i c i a l subscript end of subscript equal to E with M f i n i c i a l subscript end of subscript E P with g r a v i t a c i o n a l space i n i c i a l subscript end of subscript space plus space E with c i n e t i c a space i n i c i a l subscript end of subscript space plus space E P with e l a s t i c a i n i n i c i a l space subscript end of subscript equal to E P with g r a v i t a c i o n a l space f i n a l subscript end of subscript space more space E with c i n e t i c a f i n a l space subscript end of subscript space more E space P with e l a s t i c a f i n a l space subscript end of subscribed

at the beginning of the movement

The kinetic energy is 0 since the initial velocity is 0.
The elastic potential energy is 0 because the elastic band is not tensioned.

at the end of the movement

The gravitational potential energy is 0, relative to the length calculated at the beginning.

The balance of energies now looks like this:

E P with g r a v i t a c i o n a l i n i c i a l space subscript end of the subscript equal to E with c i n t i c a space f i n a l subscript end of subscript space plus space E P with e l a s t i c a space fin a l subscript end of subscript

Since we want speed, let's isolate kinetic energy from one side of equality.

E P with g r a v i t a c i o n a l i n i c i a l space minus subscript space end of the subscript E P with e l á s t i c a space fin a l subscript end of subscript equal to E with c i n t i c a space fin a l subscript end of subscript space

doing the calculations

gravitational potential energy

h = 15 m of natural length of the strip + 10 m of stretch = 25 m.

E P with g r a v i t a c i o n a l space i n i c i a l subscript end of the subscript equal to m. g. h E P with g r a v i t a c i o n a l space in i n i c i a l subscript end of subscript equal to 50.10.25 space equal to space 12 space 500 space J

elastic potential energy

And with P space and l a s t i c the subscript end of the subscript equal to numerator k. x squared over denominator 2 end of fraction E with P space and l á st i c a subscript end of subscript equal to numerator 250.10 squared over denominator 2 end of fraction equal to 12 space 500 J space

Replacing the values ​​in the energy balance, we have:

12 space 500 minus 12 space 500 equals E with c i n e t i c a space fin a l subscript end of subscript space 0 equals E with c i n e t i c a space fin a l subscript end of subscript space

As the kinetic energy only depends on the mass, which has not changed, and on the velocity, we have velocity equal to 0.

Identifying with calculation.

Equating the kinetic energy to 0, we have:

And with c i n is t i c a space fi n a l subscript end of subscript space equal to numerator space m. v squared over denominator 2 end of fraction equal to 0 m. v squared equal to 0 v squared equal to 0 over m v equal to 0 space

Therefore, when the strip is stretched 10 m beyond its natural length, Helena's modulus of velocity is 0 m/s.

question 11

(USP 2018) Two bodies of equal masses are released, at the same time, from rest, from height h1 and travel along the different paths (A) and (B), shown in the figure, where x1 > x2 and h1 > h2.

Consider the following statements:

I. The final kinetic energies of the bodies in (A) and (B) are different.
II. The mechanical energies of the bodies, just before they start to climb the ramp, are equal.
III. The time to complete the course is independent of the trajectory.
IV. The body in (B) reaches the end of the trajectory first.
V. The work performed by the weight force is the same in both cases.

It is correct only what is stated in

Note and Adopt: Disregard dissipative forces.

a) I and III.
b) II and V.
c) IV and V.
d) II and III.
e) I and V.

Correct answer: b) II and V.

I - WRONG: As the initial energies are equal and dissipative forces are not considered and bodies A and B go down h1 and go up h2, only the potential energy changes, equally, for both.

II - CERTA: As dissipative forces are neglected, such as friction when traveling the paths until the beginning of the climb, the mechanical energies are equal.

III - WRONG: As x1 > x2, body A travels the trajectory of the "valley", the lower part, with greater speed for a longer time. As B starts to climb first, it already loses kinetic energy, decreasing its speed. Still, after the climb, both have the same speed, but body B needs to travel a greater distance, taking longer to complete the course.

IV - WRONG: As we saw in III, body B arrives after A, as it takes longer to complete the route.

V - RIGHT: As the weight force only depends on the mass, gravity acceleration and height difference during the journey, and they are equal for both, the work performed by the weight force is the same for both.

you keep practicing with kinetic energy exercises.

you may be interested in

  • Potential energy
  • Gravitational Potential Energy
  • Elastic Potential Energy
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