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Energy · Work and power

Work

A musher pulls a sled with the rope at an angle; a worker pushes a pallet in a straight line; a cable car climbs and then descends part of the way. In all three cases there are forces and there is displacement, but the work done depends on how the two vectors combine. You are going to treat work with A-level rigour: as a scalar product, which can be calculated using either the angle or the components, and you are going to use it to predict speeds without needing to know instantaneous forces or times.

Before you start, make sure you know: Vectors in the plane (4th ESO)
Before you start, make sure you know: Kinetic energy and potential energy (4th ESO)

Work as a scalar product: $W = \vec F \cdot \vec d$

You push with all your strength against a concrete wall for ten minutes and end up exhausted, but the wall does not move; on the other hand, with a gentle push you send a skateboard rolling several metres. Why does physics say that in the first case you have done no mechanical work on the wall and in the second you have?

Of the whole force, only the component in the direction of the displacement, $F_x = F \cos \alpha$, "counts" towards the work. The perpendicular component, $F \sin \alpha$, produces no displacement in that direction and contributes no work.

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A warehouse worker pushes a pallet with a constant horizontal force of $250\ \text{N}$, moving it $12\ \text{m}$ along the floor in a straight line. a) What angle does…

A warehouse worker pushes a pallet with a constant horizontal force of $250\ \text{N}$, moving it $12\ \text{m}$ along the floor in a straight line.

  1. a) What angle does the force make with the displacement?
  2. b) Calculate the work done by the worker.
Solve
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A person walks their dog, pulling on the lead with a constant force of $80\ \text{N}$ at an angle of $60^\circ$ to the horizontal over a straight section of…

A person walks their dog, pulling on the lead with a constant force of $80\ \text{N}$ at an angle of $60^\circ$ to the horizontal over a straight section of $25\ \text{m}$ ($\cos 60^\circ = 0,5$), as shown in the figure.

F = 80 N 60° d = 25 m W = ?

Calculate the work done.

Solve

Work in components: $W = F_x \cdot d_x + F_y \cdot d_y$

In a space-navigation video game, the thrusters apply a force $\vec F = (12, -5)\ \text{N}$ to a probe while its path takes it from $(0, 0)$ to $(8, 3)\ \text{m}$, and measuring the angle between the two vectors is not practical. How can we calculate the exact energy transferred to the ship by using the coordinates of its position and of the force directly?

Graphical resolution of a force vector into Cartesian components, showing the horizontal component Fx in the same direction as the displacement d d = (dx, 0) F = (Fx, Fy) Fx
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In the laboratory, a trolley on an air track moves $\vec{d} = (5, 0)\ \text{m}$ while acted upon by a constant force $\vec{F} = (6, 8)\ \text{N}$, as shown in the…

In the laboratory, a trolley on an air track moves $\vec{d} = (5, 0)\ \text{m}$ while acted upon by a constant force $\vec{F} = (6, 8)\ \text{N}$, as shown in the figure.

x y d = (5, 0) m F = (6, 8) N Fₓ Fy
  1. a) Calculate the work using the dot product $W = \vec{F} \cdot \vec{d} = F_x \cdot d_x + F_y \cdot d_y$.
  2. b) Explain why the vertical component of the force does not contribute to the work.
Solve
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A constant force $\vec{F} = (15, -8)\ \text{N}$ acts on a machine component while the component moves through a displacement of $\vec{d} = (4, 2)\ \text{m}$, as shown in…

A constant force $\vec{F} = (15, -8)\ \text{N}$ acts on a machine component while the component moves through a displacement of $\vec{d} = (4, 2)\ \text{m}$, as shown in the figure.

x y d = (4, 2) m F = (15, −8) N Fₓ Fy
  1. a) Calculate the work using the dot product $W = \vec{F} \cdot \vec{d} = F_x \cdot d_x + F_y \cdot d_y$.
  2. b) Check that the component $F_y$ does negative work and interpret what that sign means physically.
Solve

Friction and net work on an inclined plane

Free-body diagram of a block moving up an inclined plane: pulling force and friction parallel to the ramp, normal reaction perpendicular to it, vertical weight and its component parallel to the ramp θ F pull friction N (normal) P
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To load a fridge of $60\ \text{kg}$ into a van, it is pushed up a ramp of $3\ \text{m}$ at an angle of $20^\circ$ to the horizontal ($\sen 20^\circ \approx 0,34$; take…

To load a fridge of $60\ \text{kg}$ into a van, it is pushed up a ramp of $3\ \text{m}$ at an angle of $20^\circ$ to the horizontal ($\sen 20^\circ \approx 0,34$; take $g = 10\ \text{m/s}^2$), as shown in the figure.

20° 60 kg P pₓ = ? 3 m
  1. a) Calculate the component of the weight parallel to the ramp.
  2. b) Calculate the work done by the weight during the ascent.
  3. c) What minimum work must the person pushing do against that component of weight?
Solve
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A box of $25\ \text{kg}$ starts from rest on the horizontal floor of a warehouse, where the coefficient of kinetic friction is $\mu = 0,2$. It is pushed with a constant…

A box of $25\ \text{kg}$ starts from rest on the horizontal floor of a warehouse, where the coefficient of kinetic friction is $\mu = 0,2$. It is pushed with a constant horizontal force of $100\ \text{N}$ over $12\ \text{m}$ (take $g = 10\ \text{m/s}^2$), as shown in the figure.

μ = 0,2 25 kg F = 100 N Froz = ? N P d = 12 m
  1. a) Calculate the kinetic friction force, $F_{roz} = \mu \cdot N$, taking into account that on a horizontal floor the normal force is $N = m \cdot g$.
  2. b) Calculate the work done by each of the forces (push, friction, weight, and normal force) and the net work.
  3. c) Apply the work-energy theorem to find the speed of the box at the end of the $12\ \text{m}$.
Solve

The work–energy theorem: $W_{net} = \Delta E_k$

Road-safety tests show that a car braking hard at $40\ \text{km/h}$ travels $8\ \text{m}$, but at twice the speed ($80\ \text{km/h}$) it does not need twice the distance, but $32\ \text{m}$. What physical principle links the work done by the brakes with the loss of speed of the vehicle without needing to calculate how long the braking lasts?

A car reduces its speed from v₀ to v over a distance d under a resultant force that opposes the motion; the net work of that force is equal to the decrease in kinetic energy, shown with two bars v₀ v F d ½mv₀² ½mv² Ek initial Ek final ΔEk W net = ΔEk W net: work done by the resultant force ΔEk: change in kinetic energy
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The work-energy theorem states that the net work done on a body is equal to the change in its kinetic energy:…

The work-energy theorem states that the net work done on a body is equal to the change in its kinetic energy: $W_{neto} = \Delta E_c = \frac{1}{2} \cdot m \cdot v^2 - \frac{1}{2} \cdot m \cdot v_0^2$. A demonstration ball of $2\ \text{kg}$ increases its speed from $3\ \text{m/s}$ to $5\ \text{m/s}$ on an air track.

  1. a) Calculate its initial kinetic energy and its final kinetic energy.
  2. b) What is the net work done on the ball?
Solve
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A car of $1000\ \text{kg}$ travelling at $20\ \text{m/s}$ brakes to a halt over a distance of $50\ \text{m}$ along a horizontal section. a) Calculate the change in…

A car of $1000\ \text{kg}$ travelling at $20\ \text{m/s}$ brakes to a halt over a distance of $50\ \text{m}$ along a horizontal section.

  1. a) Calculate the change in kinetic energy during braking.
  2. b) Applying the work-energy theorem, find the work done by the net braking force.
  3. c) What is the average value of this net braking force? State its sense.
Solve
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On an ice rink, a puck of mass $m$ is launched with an initial speed of $v_0 = 10\ \text{m/s}$, and slides in a straight line until coming to a stop due to friction…

On an ice rink, a puck of mass $m$ is launched with an initial speed of $v_0 = 10\ \text{m/s}$, and slides in a straight line until coming to a stop due to friction ($\mu = 0,25$; take $g = 10\ \text{m/s}^2$).

  1. a) Write the expression for the work done by friction and, applying the work-energy theorem, obtain the stopping distance $d$ as a function of $v_0$, $\mu$, and $g$.
  2. b) Calculate this distance numerically.
  3. c) Reason, from the expression obtained, whether the stopping distance depends on the mass of the puck. What practical implication does this result have for road safety?
Solve

The work done by weight does not depend on the path

Path of a cable car going up from 1200 m to 1750 m and down to 1550 m: the work done by the weight depends only on the net change in height of 350 m between departure and arrival Net Δh = 350 m base · 1200 m summit · 1750 m intermediate · 1550 m ascent: +550 m descent: −200 m
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A cable car cabin with its passengers has a total mass of $800\ \text{kg}$. On the outbound journey, it ascends from the base station, at an altitude of…

A cable car cabin with its passengers has a total mass of $800\ \text{kg}$. On the outbound journey, it ascends from the base station, at an altitude of $1200\ \text{m}$, to the top station, at $1750\ \text{m}$. It then partially descends to an intermediate station located at $1550\ \text{m}$ (take $g = 10\ \text{m/s}^2$), as shown in the figure.

base · 1200 m top · 1750 m intermediate · 1550 m W total = ?
  1. a) Calculate the work done by weight during the ascent.
  2. b) Calculate the work done by weight during the partial descent.
  3. c) Calculate the total work done by weight over the entire journey and verify that it depends only on the net difference in altitude between the starting and ending points. What property of the gravitational force does this result highlight?
Solve
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An elevator cabin with its passengers has a mass of $600\ \text{kg}$. It starts from rest and ascends $12\ \text{m}$ with a constant acceleration of $1,2\ \text{m/s}^2$…

An elevator cabin with its passengers has a mass of $600\ \text{kg}$. It starts from rest and ascends $12\ \text{m}$ with a constant acceleration of $1,2\ \text{m/s}^2$ (take $g = 10\ \text{m/s}^2$).

  1. a) Calculate the force exerted by the cable applying Newton's second law: $T - m \cdot g = m \cdot a$.
  2. b) Calculate the work done by the cable and the work done by weight during these $12\ \text{m}$.
  3. c) Find the net work and, using the work-energy theorem, the speed of the cabin after $12\ \text{m}$. Check the result using kinematics: $v^2 = 2 \cdot a \cdot h$.
Solve

Back to the start: for the musher's sled, only the horizontal component of the rope does useful work ($F \cos\alpha$); for the pallet pushed in a straight line, the whole force is parallel to the displacement (maximum work with $\alpha=0^\circ$); and for the cable car, the work done by the weight depends only on the net change in height between departure and arrival, regardless of the intermediate ascents and descents.

Summary

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