Forces

Free body diagrams are a technique that helps visualize the force vectors used to solve Newton's second law.

m F F m F F F F F F m F m F F F

A free body diagram shows all the force vectors on an object. Mass is typically written inside a box, with force vectors pointed away from the box.

Example: Draw a free body diagram for a 83 kg person holding onto a rope in a game of "Tug of war". The rope is pulling them with a force of 520 N left. The person's feet are countering that with 540 N to the right.
solution 83 kg 520 N 540 N
2.0 kg 200 N 500 N 300 N Example: Use the free body diagram to calculate the mass's acceleration.
solution $$\sum F=ma$$ $$-200\,\mathrm{N}+300\,\mathrm{N}+500\,\mathrm{N}=ma$$ $$600\,\mathrm{N}=(2\,\mathrm{kg})a$$ $$300 \mathrm{\tfrac{m}{s^2}}=a$$
0.09 kg 0.34 N F= ? Example: The book The Martian by Andy Weir (mass = 0.09 kg) is resting on a table (acceleration = zero). The force of gravity produces a downwards force of 0.34 N. What force is required to keep the book at rest on the table?
solution $$\sum F=ma$$ $$F_{N} + F_{g} = ma$$ $$F_{N} - 0.34\, \mathrm{N} = (0.09\, \mathrm{kg})(0)$$ $$F_{N} - 0.34\,\mathrm{N} = 0$$ $$F_{N} = 0.34 \, \mathrm{N}$$
16 kg 85 N 22 N 140 N 55 N 78 N Example: Use the free body diagram to calculate the acceleration for both the horizontal and the vertical.
solution $$ \text{vertical}$$ $$\sum F=ma$$ $$22 \, \mathrm{N} - 85 \, \mathrm{N} = (16 \, \mathrm{kg})a$$ $$-63 \, \mathrm{N} = (16 \, \mathrm{kg})a$$ $$-3.9 \, \mathrm{\tfrac{m}{s^2}} = a$$
$$ \text{horizontal}$$ $$\sum F=ma$$ $$78 \, \mathrm{N}+55 \, \mathrm{N}-140 \, \mathrm{N} = (16 \, \mathrm{kg})a$$ $$-7 \, \mathrm{N} = (16 \, \mathrm{kg})a$$ $$-0.43 \, \mathrm{\tfrac{m}{s^2}} = a$$
Example: A red crate is falling, but a parachute is slowing its acceleration to only 2 m/s² down. The force of gravity is 833 N down. The parachute provides 663 N up. Draw a free body diagram and use it to find the mass of the crate.
solution m = ? 833 N 663 N $$\sum F=ma$$ $$F_1+F_2=ma$$ $$-833+663 = m(2)$$ $$\frac{-170}{2} = \frac{m(2)}{2}$$ $$-85 \, \mathrm{kg} = m$$

A negative mass doesn't make sense. Where did we mess up?
Oh, the acceleration is negative, because it points down.

$$\frac{-170}{-2} = \frac{m(-2)}{-2}$$ $$85 \, \mathrm{kg} = m$$

The Force of gravity

Mass is a measure of an object's inertia. Mass also determines the strength of gravity. Because of gravity all objects are attracted to each other, but we mostly notice the attraction towards the Earth because it is so large and so close.

There is a special word to describe the direction of gravity, down.


m F g

$$F_g=mg $$

\(F_g\) = the force of gravity, weight [N, newtons, kg m/s²] vector
\(m\) = mass [kg]
\(g\) = acceleration of gravity on Earth = 9.8 [m/s²] vector

The force of gravity depends only on the mass of the object because on the surface of the Earth acceleration from gravity is the same for all objects. If you aren't on the surface of the Earth, there is a different way to calculate gravity.

Question: Why do feathers fall slower than bricks?
answer

Air friction produces a force that opposes motion. Feathers have a large surface area compared to their small mass so they have more air friction.

The acceleration of 9.8 m/s² on the surface of the Earth is just an approximation. The gravity of Earth changes a bit depending on where you are.

Table: Comparative gravities in various cities around the world
Location Acceleration in m/s² Acceleration in ft/s²
Amsterdam 9.813 32.19
Athens 9.800 32.15
Auckland 9.799 32.15
Bangkok 9.783 32.1
Brussels 9.811 32.19
Buenos Aires 9.797 32.14
Calcutta 9.788 32.11
Cape Town 9.796 32.14
Chicago 9.803 32.16
Copenhagen 9.815 32.2
Frankfurt 9.810 32.19
Havana 9.788 32.11
Helsinki 9.819 32.21
Istanbul 9.808 32.18
Jakarta 9.781 32.09
Kuwait 9.793 32.13
Lisbon 9.801 32.16
London 9.812 32.19
Los Angeles 9.796 32.14
Madrid 9.800 32.15
Manila 9.784 32.1
Mexico City 9.779 32.08
Montréal 9.789 32.12
New York City 9.802 32.16
Nicosia 9.797 32.14
Oslo 9.819 32.21
Ottawa 9.806 32.17
Paris 9.809 32.18
Rio de Janeiro 9.788 32.11
Rome 9.803 32.16
San Francisco 9.800 32.15
Singapore 9.781 32.09
Skopje 9.804 32.17
Stockholm 9.818 32.21
Sydney 9.797 32.14
Taipei 9.790 32.12
Tokyo 9.798 32.15
Vancouver 9.809 32.18
Washington, D.C. 9.801 32.16
Wellington 9.803 32.16
Zurich 9.807 32.18

Question: What factors might explain why the measured acceleration of gravity changes in different locations on the surface of Earth?
answer

  • Gravity is slightly weaker at higher elevation because you are farther from the center of the Earth.

  • Near the equator gravity feels weaker because the Earth's rotation adds a centrifugal force.
  • The Three-Body Problem Example: The Three-Body Problem by Cixin Liu has a mass of 0.44 kg. What force of gravity does the book have?
    solution $$F_g=mg$$ $$F_g=(0.44 \, \mathrm{kg} )(9.8\, \mathrm{\tfrac{m}{s^2}})$$ $$F_g=4.3 \, \mathrm{N}$$
    Cat's Cradle Example: How much mass does the book Cat's Cradle by Kurt Vonnegut have if it feels a force of gravity of 1.8 N?
    solution $$F_g=mg$$ $$1.8=m(9.8)$$ $$\frac{1.8}{9.8}=m$$ $$0.18 \, \mathrm{kg}=m$$

    Weight and Mass

    Another word for the force of gravity is weight. An object on the Moon would weigh less than it does on Earth because of the lower gravity, but it would still have the same mass.

    $$F_g = \mathrm{weight}$$

    Earth's gravity does extend into space, but it decreases with distance. It is about ~90% for astronauts in orbit around the Earth, but they don't notice any gravity because they are in a freefall.

    Freefall means that you are just letting gravity accelerate you without any opposing forces. To keep from falling we are careful to always counter the force of gravity. This can be done with a parachute, or a jet pack, or just the ground.

    Ducks: Two Years in the Oil Sands Question: Ducks: Two Years in the Oil Sands by Kate Beaton has a mass of 1.14 kg. How does its mass and weight change in a freefall on Earth?
    answer

    An object's mass doesn't change when it is falling.

    Weight just means the force of gravity, which also doesn't change in a short freefall.

    Seveneves Example: The hardcover version of Seveneves by Neal Stephenson has a mass of 0.95 kg. What is the force of gravity felt by the book on Earth? What about on the Moon?
    Local Massive Objects Surface Gravity
    name g (m/s²)
    Sun 275
    Mercury 3.7
    Venus 8.9
    Earth 9.8
    Moon 1.6
    Mars 3.7
    Jupiter 25.8
    Saturn 10.4
    Uranus 8.7
    Neptune 11.2
    solution

    Weight and force of gravity mean the same thing. A planet's gravity field determines your weight, but not your mass.

    • $$\text{Earth}$$ $$F_{g}=mg$$ $$F_{g}=(0.95)(9.8)$$ $$F_{g}=9.31 \, \mathrm{N}$$
    • $$\text{Moon}$$ $$F_{g}=mg$$ $$F_{g}=(0.95)(1.6)$$ $$F_{g}=1.52 \, \mathrm{N}$$
    Converting kilograms (kg) into pounds (lbs) $$1 \, \mathrm{kg} = 2.2\, \mathrm{lbs} \quad \scriptsize \text{(On Earth)}$$ $$1 \, \mathrm{N} = 0.2248\, \mathrm{lbs}$$

    Pounds are a unit of force and kilograms are a unit of mass. You can't convert directly between them because they are different concepts, but you can use the force of gravity equation to find a conversion that works for only Earth's surface.

    Uprooted Example: Uprooted by Naomi Novik is resting on a table. The shipping weight is 1.2 pounds. What is the book's mass in kilograms on Earth? On Mars?
    solution

    Mass doesn't depend on gravity, so it's the same everywhere.

    $$ 1.2\,\mathrm{lbs} \left( \frac{1\,\mathrm{kg}}{2.2\,\mathrm{lbs}} \right)= 0.\overline{54}\,\mathrm{kg}$$ $$ m = 0. \overline{54} \, \mathrm{kg} $$

    What is the weight of the book in Newtons on Earth? On Mars?
    solution
    • $$\text{weight on Earth}$$ $$F_{g}=mg$$ $$F_{g}=(0.\overline{54})(9.8)$$ $$F_{g}=5.35\, \mathrm{N}$$
    • $$\text{weight on Mars}$$ $$F_{g}=mg$$ $$F_{g}=(0.\overline{54})(3.711)$$ $$F_{g}=2.02\, \mathrm{N}$$

    The Normal Force

    Typically a normal force will balance the force of gravity to keep an object from accelerating up or down.

    m F N F g

    A normal force occurs when two objects are in contact. It is perpendicular to the point of contact. A normal force prevents objects from passing through each other.

    A normal force will scale to a value that will keep the net force and acceleration zero.

    Normal forces come from the combined effect of electromagnetic forces and the Pauli exclusion principle.

    The electromagnetic force allows chemical bonds to form. These bonds give solid matter its rigid structure, which is required for normal forces.

    At the atomic scale, particles can't pass through each other primarily because of a quantum mechanical effect called the Pauli exclusion principle . The Pauli exclusion principle is mostly responsible for keeping particles, like electrons, separate.

    m

    Press E to activate the mass. Then press WASD to apply forces to the mass. Imagine that gravity is pointed towards the bottom of the page.

    Question: What force keeps the mass from exiting the screen?
    answer

    The normal force.


    Question: Why does pressing A and D at the same time do nothing?
    answer

    The left and right force cancel each other out.

    Example: You are accelerating up in an elevator at 2 m/s². If your mass is 100 kg, what is the normal force you feel from the elevator?
    solution 100 kg F g = 980 N F N = ? $$F_{g}=mg$$ $$F_{g}=(100)(9.8)$$ $$F_{g}=980\, \mathrm{N}$$
    $$\sum F=ma$$ $$F_{N}-F_{g}=ma$$ $$F_{N} - 980=(100)(2)$$ $$F_{N}=1180\, \mathrm{N}$$
    Example: A 20 kg box is at rest on a horizontal sidewalk. Find the force of gravity and the normal force on the box.
    solution

    In the simple case of a flat horizontal surface with no vertical acceleration the force of gravity will always be equal and opposite to the normal force.

    20 kg F N F g $$F_{g}=mg$$ $$F_{g}=(20)(9.8)$$ $$F_{g}=196\, \mathrm{N}$$
    $$\sum F=ma$$ $$F_{N}-F_{g}=ma$$ $$F_{N} - 196=(20)(0) $$ $$F_{N}=196 \, \mathrm{N}$$
    20 kg F N Fg Example: A 20 kg box is at rest on a steep sidewalk. The sidewalk is at an angle 20 degrees from horizontal. Find the force of gravity and the normal force on the box. What is the acceleration of the box? (assume no friction)
    solution
    • $$F_{g}=mg$$ $$F_{g}=(20)(9.8)$$ $$F_{g}=196 \, \mathrm{N}$$

    • Fg Fg⊥ Fg∥

    Separate the gravity vector into components parallel and perpendicular to the ground. Acceleration is zero in the perpendicular direction.

    • $$\text{perpendicular to ground}$$

      $$F_{g\perp}=F_{g}\cos(20)$$ $$F_{g\perp}=(196)\cos(20)$$ $$F_{g\perp}=184 \, \mathrm{N}$$
      $$\sum F_{\perp}=ma$$ $$-F_{g\perp}+F_{N}=ma$$ $$-184+F_N=(20)(0)$$ $$F_N=184$$ $$F_{N}=184 \, \mathrm{N}$$
    • $$\text{parallel to ground}$$

      $$F_{g\parallel}=F_{g}\sin(20)$$ $$F_{g\parallel}=(196)\sin(20)$$ $$F_{g\parallel}=67 \, \mathrm{N}$$
      $$\sum F_{\parallel}=ma$$ $$F_{g\parallel}=ma$$ $$(67)=(20)a$$ $$3.35 \, \mathrm{\tfrac{m}{s^{2}}}=a$$
    20 kg F N = 184 N Fg = 196 N

    Tension Forces

    When a person is walking a dog they are able to apply a force on the dog with a leash. They use the tension on the leash to transfer that force from their hand to the dog.

    T T

    Tension is the pulling force from a chain, string, or rope. Tension is useful for transferring a force over a distance. In most situations, the tension is the same for both ends.

    Example: A helium balloon is attached to a 0.5 g paper clip. If the balloon and paper clip are accelerating up at 0.023 m/s², what is the tension on the paper clip from the balloon in Newtons?
    solution 0.0005 kg T F g $$\sum F=ma$$ $$-F_{g} + T = ma$$ $$-(0.0005)(9.8)+T=(0.0005)(0.023)$$ $$-0.0049+T=0.0000115$$ $$T=0.0000115+0.0049$$ $$T = 0.0049115\, \mathrm{N}$$
    Example: A 100 kg person is pulling a 10 kg crate with a rope (ignore the mass of the rope). Both the person and the crate are accelerating to the left at 0.1 m/s². What force is the person producing in order to accelerate to the left?
    solution 100 kg F person T 10 kg T

    The tension force is equal and opposite for the person and crate.

    $$\text{crate on right}$$ $$\sum F=ma$$ $$T = 10 (-0.1)$$ $$T = \color{#f05}-1 \, \mathrm{N}$$
    $$\text{person on left}$$ $$\sum F=ma$$ $$F_{\mathrm{person}} + T = ma$$ $$F_{\mathrm{person}} {\color{#f05}+ 1 \, \mathrm{N}} = (100 \, \mathrm{kg})(-0.1\, \mathrm{\tfrac{m}{s^2}})$$ $$F_{\mathrm{person}} + 1\, \mathrm{N} = -10\, \mathrm{N}$$ $$F_{\mathrm{person}} = -11\,\mathrm{N}$$
    T x 10 kg T F dog Example: You are walking your dog with the leash at a 45 degree angle down towards the dog. Neither you nor the dog are accelerating. The dog is pulling on the leash forward with a force of 100 N. Calculate the x part of the tension force on the leash. Then calculate the total tension force.
    solution $$\text{dog: horizontal}$$ $$\sum F=ma$$ $$-T_x + F_{\mathrm{dog}} = 0$$ $$-T_x + 100 \, \mathrm{N} = 0$$ $$T_x= 100 \,\mathrm{N}$$

    The 100 N is only the x-part of the tension force vector. We can find the total tension force with the Pythagorean theorem. At 45° the x and y parts of the force are the same.

    $$T^2 = 100^2+100^2$$ $$T^2 = 20\,000$$ $$T = 141 \, \mathrm{N}$$
    0.4 kg F 10 kg Example: A 0.4 kg squirrel is pulling a 10 kg box with a string. The squirrel and box are accelerating to the left at 0.5 m/s². What is the force of tension on the string? What force is the squirrel producing in order to accelerate to the left?
    solution $$ \text{box}$$ $$\sum F=ma$$ $$F_{\mathrm{tension}}=(10)(-0.5)$$ $$F_{\mathrm{tension}}=-5\, \mathrm{N}$$

    The tension force on the string is equal but opposite for the squirrel and box.

    $$ \text{squirrel}$$ $$\sum F=ma$$ $$F_{\mathrm{squirrel}} + F_{\mathrm{tension}}=ma$$ $$F_{\mathrm{squirrel}} + 5=(0.4)(-0.5)$$ $$F_{\mathrm{squirrel}}=-0.2-5$$ $$F_{\mathrm{squirrel}}=-5.2 \, \mathrm{N}$$

    The negative sign tells us that the squirrel's force is pointed left.

    $$F_{\mathrm{squirrel}}=5.2 \, \mathrm{N} \text{ left}$$
    20 kg 10 kg T T Example: Use the diagram to predict the acceleration of the masses.
    Assume no friction, no air resistance, Earth gravity, and a massless rope.
    hint
    20 kg T = ? F N F g 10 kg T = ? F g = ?

    Both free body diagrams share the same tension and acceleration. Build two equations with Newton's second law and solve a system of equations for T and a. While T and a are the same magnitude they have different directions, so watch the sign of acceleration in particular.

    This Khan academy video covers this problem in more depth.

    solution $$\text{20kg box: horizontal}$$ $$\sum F=ma_x$$ $$T = ma_x$$ $$T = \color{#d3a}20a_x$$
    $$\text{10kg box: vertical}$$ $$\sum F=ma_y$$ $$T - F_g = ma_y$$ $$T - mg = ma_y$$ $$T - (10)(9.8) = 10a_y$$
    $${\color{#d3a}20a_x} - 98 = 10a_y$$
    $$a_x = -a_y$$
    $${\color{#d3a}-20a_y} - 98 = 10a_y$$ $$-98 = 10a_y + 20a_y$$ $$-98 = 30a_y$$ $$-3.2\overline{6} \, \mathrm{\tfrac{m}{s^2}} = a_y$$
    solution (treating system as one mass) $$\text{gravity only pulls on the 10kg part}$$ $$F_g = m g$$ $$F_g = (10 \, \mathrm{kg})(9.8\, \mathrm{\tfrac{m}{s^2}})$$ $$F_g = \color{#d3a}98 \, \mathrm{N}$$
    $$\text{use both masses to find acceleration in the vertical}$$ $$\sum F=ma$$ $$F_g = (10\, \mathrm{kg}+20\, \mathrm{kg}) a$$ $$F_g = (30\, \mathrm{kg}) a$$ $$98\, \mathrm{N} = (30\,\mathrm{kg}) a$$ $$-3.2\overline{6} \, \mathrm{\tfrac{m}{s^2}}= a$$
    10 kg 25 kg Example: Two blocks are attached to each other with a rope hanging over a wheel. Find the acceleration of each body. Ignore friction, and assume the wheel and rope have a negligible mass.
    solution
    $$\text{10 kg block}$$ $$\sum F = ma$$ $$T-mg = ma$$ $$T-(10)(9.8) = ma$$ $$T-98 = 10a$$ $$T = 10a+98$$
    $$\text{25 kg block}$$ $$\sum F = ma$$ $$T-mg = ma$$ $$T-(25)(9.8) = 25a$$ $$T-245 = 25a$$ $$T = 25a+245$$

    We have two variables and two equations, this means we can plug one equation into the other. The Tension is the same for each body. The accelerations are the same, but in opposite directions, so we need to make one acceleration negative.

    $$T = 10({\color{#f05}-a})+98$$
    $$T = 25a+245$$
    $$10({\color{#f05}-a})+98 = 25a+245 $$ $$-35a = 147$$ $$a = -4.2 \, \tfrac{m}{s^2}$$

    The 25kg object is falling down at 4.2 m/s². The 10kg is rising up at 4.2 m/s².

    practice problems (28)

    In case you wanted more practice I used AI to make some more problems. The rest of the site I made by hand, but generating endless problems seemed safe. I did find mistakes in the AI generated problems, and there are probably some I didn't find. Let me know if something could be fixed. I also added a practice problem on each page with no solution. That's intentional. Have fun!

    Unless a problem says otherwise, assume Earth gravity, no air resistance, no friction, and massless ropes.

    printout.pdf

    Example: A 6.0 kg box has three horizontal forces on it: 18 N right, 10 N left, and 4.0 N right. What is the box's horizontal acceleration?
    solution 6.0 kg 18 N 4.0 N 10 N

    Let right be positive.

    $$\sum F = 18 - 10 + 4.0$$ $$\sum F = 12\,\mathrm{N}$$
    $$\sum F = ma$$ $$12 = 6.0a$$ $$a = \frac{12}{6.0}$$ $$a = 2.0\,\mathrm{\tfrac{m}{s^{2}}}$$

    The box accelerates to the right.

    Example: A kitchen scale shows that a textbook has a mass of 1850 g. The book rests on a flat table. What are the force of gravity and the normal force on the book?
    solution $$1850\,\textcolor{DeepPink}{\mathrm{g}}\left(\frac{1\,\mathrm{kg}}{1000\,\textcolor{DeepPink}{\mathrm{g}}}\right)$$ $$1.85\,\mathrm{kg}$$
    $$F_g = mg$$ $$F_g = (1.85)(9.8)$$ $$F_g = 18.1\,\mathrm{N}$$

    The book isn't accelerating up or down, so the vertical forces cancel. Let up be positive.

    $$\sum F = ma$$ $$F_N - F_g = ma$$ $$F_N - 18.1 = (1.85)(0)$$ $$F_N = 18.1\,\mathrm{N}$$
    Question: A textbook rests on a table. The normal force on the book is equal and opposite to the book's weight. Are these two forces a Newton's third law pair?
    answer

    No. Both forces act on the same object, the book. Third law pairs always act on two different objects.

    The third law partner of the book's weight is the book pulling up on the Earth. The partner of the normal force is the book pushing down on the table. The weight and normal force are equal here only because the book isn't accelerating. In an accelerating elevator they would be different.

    Example: An 80 kg person rides an elevator up to the 12th floor. At the start of the ride, the elevator accelerates upward at 1.5 m/s². What normal force does the floor apply to the person?
    solution 80 kg F N = 904 N F g = 784 N

    Let up be positive.

    $$m = 80\,\mathrm{kg}$$ $$a = 1.5\,\mathrm{\tfrac{m}{s^{2}}}$$ $$F_N = \,?$$
    $$F_g = mg$$ $$F_g = (80)(9.8)$$ $$F_g = 784\,\mathrm{N}$$
    $$\sum F = ma$$ $$F_N - F_g = ma$$ $$F_N - 784 = (80)(1.5)$$ $$F_N - 784 = 120$$ $$F_N = 904\,\mathrm{N}$$

    The floor pushes up harder than the person's weight. That extra push is what you feel when an elevator starts going up.

    Example: A 60 kg person stands in an elevator accelerating downward at 2.0 m/s². What normal force does the floor apply to the person?
    solution

    Let up be positive, so the acceleration is negative.

    $$m = 60\,\mathrm{kg}$$ $$a = -2.0\,\mathrm{\tfrac{m}{s^{2}}}$$ $$F_N = \,?$$
    $$F_g = mg$$ $$F_g = (60)(9.8)$$ $$F_g = 588\,\mathrm{N}$$
    $$\sum F = ma$$ $$F_N - F_g = ma$$ $$F_N - 588 = (60)(-2.0)$$ $$F_N - 588 = -120$$ $$F_N = 468\,\mathrm{N}$$

    The normal force is less than the person's weight, so they feel lighter for a moment.

    Example: An elevator is slowing down as it approaches the top floor. At one moment it is moving upward at 3.0 m/s. What is the normal force on a 20 kg box sitting on the elevator floor?
    solution

    This cannot be solved from the information given. The normal force depends on the elevator's acceleration, not its velocity. We know the elevator is slowing down, so the acceleration points down, but we don't know how large it is.

    We can say the normal force is less than the box's 196 N weight. If the elevator were moving at a constant 3.0 m/s, the normal force would be exactly 196 N.

    Example: At the airport, a bag scale says your backpack weighs 22 pounds. What is the backpack's mass in kilograms, and what is its weight in newtons? (1 kg = 2.2 lbs on Earth)
    solution $$22\,\textcolor{DeepPink}{\mathrm{lbs}}\left(\frac{1\,\mathrm{kg}}{2.2\,\textcolor{DeepPink}{\mathrm{lbs}}}\right)$$ $$10\,\mathrm{kg}$$
    $$F_g = mg$$ $$F_g = (10)(9.8)$$ $$F_g = 98\,\mathrm{N}$$

    Pounds measure force, like newtons. The kilogram conversion only works on Earth's surface.

    Example: A 3.0 kg rock is taken to the Moon and to Mars. What is its weight on each world? Use 1.6 m/s² for the Moon and 3.711 m/s² for Mars.
    solution
    $$\text{Moon}$$ $$F_g = mg$$ $$F_g = (3.0)(1.6)$$ $$F_g = 4.8\,\mathrm{N}$$
    $$\text{Mars}$$ $$F_g = mg$$ $$F_g = (3.0)(3.711)$$ $$F_g = 11.1\,\mathrm{N}$$

    The rock's mass is 3.0 kg everywhere. Only its weight changes, because the gravity changes.

    Example: A rover scoops up a rock sample on Mars, where gravity is 3.711 m/s². The rover measures the sample's weight as 22.3 N. What is the sample's mass?
    solution $$F_g = 22.3\,\mathrm{N}$$ $$g = 3.711\,\mathrm{\tfrac{m}{s^{2}}}$$ $$m = \,?$$
    $$F_g = mg$$ $$22.3 = m(3.711)$$ $$m = \frac{22.3}{3.711}$$ $$m = 6.01\,\mathrm{kg}$$

    Back on Earth, the same 6.01 kg sample would weigh 58.9 N.

    Example: A supply crate is dropped from a helicopter with a small parachute. The crate's weight is 686 N, and the parachute pulls up on it with 196 N. What are the crate's mass and acceleration?
    solution $$F_g = mg$$ $$686 = m(9.8)$$ $$m = \frac{686}{9.8}$$ $$m = 70\,\mathrm{kg}$$

    Let up be positive.

    $$\sum F = ma$$ $$196 - 686 = 70a$$ $$-490 = 70a$$ $$a = \frac{-490}{70}$$ $$a = -7.0\,\mathrm{\tfrac{m}{s^{2}}}$$

    The crate still speeds up as it falls, but more slowly than it would in free fall.

    Example: An 85 kg skydiver has reached terminal velocity, so they are falling at a constant speed. What upward force does air resistance apply to the skydiver?
    solution

    Constant speed means the acceleration is zero, so the forces balance.

    $$F_g = mg$$ $$F_g = (85)(9.8)$$ $$F_g = 833\,\mathrm{N}$$
    $$\sum F = ma$$ $$F_{\mathrm{air}} - F_g = 0$$ $$F_{\mathrm{air}} - 833 = 0$$ $$F_{\mathrm{air}} = 833\,\mathrm{N}$$

    The skydiver is falling fast, but the net force is zero.

    Example: A 10 kg box slides down a smooth 30° loading ramp. Assume no friction. Find the force of gravity, the normal force, the component of gravity down the ramp, and the box's acceleration.
    solution $$F_g = mg$$ $$F_g = (10)(9.8)$$ $$F_g = 98\,\mathrm{N}$$

    Make sure your calculator is in degree mode. Split gravity into components perpendicular and parallel to the ramp.

    $$\text{perpendicular to ramp}$$ $$F_{g\perp} = F_g\cos(30\degree)$$ $$F_{g\perp} = (98)\cos(30\degree)$$ $$F_{g\perp} = 84.9\,\mathrm{N}$$ $$F_N = 84.9\,\mathrm{N}$$
    $$\text{parallel to ramp}$$ $$F_{g\parallel} = F_g\sin(30\degree)$$ $$F_{g\parallel} = (98)\sin(30\degree)$$ $$F_{g\parallel} = 49.0\,\mathrm{N}$$
    $$\sum F = ma$$ $$49.0 = 10a$$ $$a = 4.9\,\mathrm{\tfrac{m}{s^{2}}}$$

    On a ramp, the normal force is less than the weight.

    Example: The page's example found that a 20 kg box on a frictionless 20° hill accelerates at 3.35 m/s². A 60 kg adult on a sled slides down the same frictionless hill. What are the adult's normal force and acceleration?
    solution $$F_g = mg$$ $$F_g = (60)(9.8)$$ $$F_g = 588\,\mathrm{N}$$
    $$\text{perpendicular}$$ $$F_N = F_g\cos(20\degree)$$ $$F_N = (588)\cos(20\degree)$$ $$F_N = 553\,\mathrm{N}$$
    $$\text{parallel}$$ $$F_{g\parallel} = F_g\sin(20\degree)$$ $$F_{g\parallel} = (588)\sin(20\degree)$$ $$F_{g\parallel} = 201\,\mathrm{N}$$
    $$\sum F = ma$$ $$201 = 60a$$ $$a = 3.35\,\mathrm{\tfrac{m}{s^{2}}}$$

    The adult has the same acceleration as the 20 kg box. A heavier object has a bigger force down the hill, but it also has more mass to accelerate, so the mass cancels. It's the same reason all objects fall at 9.8 m/s².

    Example: A 1.2 kg camera drone hovers in a gusty wind. Its rotors push it straight up with 15 N, and the wind pushes it sideways with 3.0 N. Find the drone's horizontal and vertical acceleration.
    solution 1.2 kg 15 N F g = 11.8 N 3.0 N $$F_g = mg$$ $$F_g = (1.2)(9.8)$$ $$F_g = 11.8\,\mathrm{N}$$
    $$\text{vertical}$$ $$\sum F = ma$$ $$15 - 11.8 = 1.2a$$ $$3.2 = 1.2a$$ $$a = 2.7\,\mathrm{\tfrac{m}{s^{2}}}$$
    $$\text{horizontal}$$ $$\sum F = ma$$ $$3.0 = 1.2a$$ $$a = \frac{3.0}{1.2}$$ $$a = 2.5\,\mathrm{\tfrac{m}{s^{2}}}$$

    The drone accelerates upward and sideways at the same time. Each direction is solved separately, like 2-D motion on the kinematics page.

    Example: A 4.0 kg lamp hangs motionless from a vertical cable. What is the tension in the cable?
    solution

    The lamp isn't accelerating, so the net force is zero. Let up be positive.

    $$F_g = mg$$ $$F_g = (4.0)(9.8)$$ $$F_g = 39.2\,\mathrm{N}$$
    $$\sum F = ma$$ $$T - F_g = 0$$ $$T - 39.2 = 0$$ $$T = 39.2\,\mathrm{N}$$
    Example: A 15 kg crate is lifted by a rope, and it accelerates upward at 1.2 m/s². What is the tension in the rope?
    solution

    Let up be positive.

    $$F_g = mg$$ $$F_g = (15)(9.8)$$ $$F_g = 147\,\mathrm{N}$$
    $$\sum F = ma$$ $$T - F_g = ma$$ $$T - 147 = (15)(1.2)$$ $$T - 147 = 18$$ $$T = 165\,\mathrm{N}$$

    The rope has to hold up the crate's weight and also provide the extra 18 N that accelerates it.

    Example: A 12 kg crate is lowered by a rope, and it accelerates downward at 0.75 m/s². What is the tension in the rope?
    solution

    Let up be positive, so the acceleration is negative.

    $$F_g = mg$$ $$F_g = (12)(9.8)$$ $$F_g = 117.6\,\mathrm{N}$$
    $$\sum F = ma$$ $$T - F_g = ma$$ $$T - 117.6 = (12)(-0.75)$$ $$T - 117.6 = -9$$ $$T = 109\,\mathrm{N}$$

    The tension is less than the weight, which lets the crate speed up as it goes down.

    Example: A dog pulls forward with 80 N. The leash angles back and up from the dog at 30° above the horizontal. The dog isn't accelerating. What is the total tension in the leash?
    solution dog 80 N T = 92.4 N T x = 80 N 30°

    The dog isn't accelerating, so the horizontal part of the tension balances the dog's pull.

    $$T_x = 80\,\mathrm{N}$$

    The angle is measured from the horizontal, so the horizontal part is the adjacent side.

    $$T_x = T\cos(30\degree)$$ $$80 = T\cos(30\degree)$$ $$T = \frac{80}{\cos(30\degree)}$$ $$T = 92.4\,\mathrm{N}$$

    The total tension is bigger than 80 N because part of it pulls up on the dog instead of back.

    Example: A 30 kg cart pulls a 10 kg cart with a rope on a frictionless floor. A student pulls the 30 kg cart forward with 80 N. What is the acceleration of the carts, and what is the tension in the rope between them?
    solution

    Treat both carts as one system to find the acceleration.

    $$\sum F = ma$$ $$80 = (30 + 10)a$$ $$80 = 40a$$ $$a = 2.0\,\mathrm{\tfrac{m}{s^{2}}}$$

    Now look only at the 10 kg cart. The rope tension is the only horizontal force on it.

    $$\sum F = ma$$ $$T = (10)(2.0)$$ $$T = 20\,\mathrm{N}$$

    The rope only pulls with 20 N. The other 60 N of the student's pull goes into accelerating the 30 kg cart.

    Example: A 12 kg block on a frictionless table is connected by a rope over a pulley to a hanging 4.0 kg block. What are the acceleration and the rope tension?
    solution

    Only the hanging block's weight pulls the system. Both masses have to accelerate.

    $$F_g = mg$$ $$F_g = (4.0)(9.8)$$ $$F_g = 39.2\,\mathrm{N}$$
    $$\sum F = ma$$ $$39.2 = (12 + 4.0)a$$ $$39.2 = 16a$$ $$a = 2.45\,\mathrm{\tfrac{m}{s^{2}}}$$

    The table block is pulled only by the tension.

    $$T = ma$$ $$T = (12)(2.45)$$ $$T = 29.4\,\mathrm{N}$$

    The tension is less than the hanging block's 39.2 N weight. If they were equal, the hanging block wouldn't accelerate.

    Example: Two hanging masses are connected by a rope over a frictionless pulley. One mass is 8.0 kg and the other is 5.0 kg. What are the acceleration and the rope tension?
    solution

    The heavier mass moves down and the lighter mass moves up. The difference in their weights drives the system.

    $$\sum F = (8.0)(9.8) - (5.0)(9.8)$$ $$\sum F = 29.4\,\mathrm{N}$$
    $$\sum F = ma$$ $$29.4 = (8.0 + 5.0)a$$ $$29.4 = 13a$$ $$a = 2.26\,\mathrm{\tfrac{m}{s^{2}}}$$

    Use the 5.0 kg mass, which accelerates upward, to find the tension.

    $$T - F_g = ma$$ $$T - (5.0)(9.8) = (5.0)(2.26)$$ $$T - 49 = 11.3$$ $$T = 60.3\,\mathrm{N}$$

    The tension falls between the two weights, 49 N and 78.4 N.

    Example: An 18 kg box is held at rest on a frictionless 25° ramp by a rope that pulls up along the ramp. What are the tension and the normal force?
    solution 18 kg F N = 160 N T = 74.5 N F g = 176 N $$F_g = mg$$ $$F_g = (18)(9.8)$$ $$F_g = 176.4\,\mathrm{N}$$
    $$\text{parallel to ramp}$$ $$T = F_g\sin(25\degree)$$ $$T = (176.4)\sin(25\degree)$$ $$T = 74.5\,\mathrm{N}$$
    $$\text{perpendicular to ramp}$$ $$F_N = F_g\cos(25\degree)$$ $$F_N = (176.4)\cos(25\degree)$$ $$F_N = 160\,\mathrm{N}$$

    The rope only has to hold back the part of gravity that points down the ramp, which is much less than the box's full weight.

    Example: A 70 kg person stands on a bathroom scale in an elevator. Scales measure the normal force and then divide by 9.8 to display kilograms. As the elevator starts moving, the scale reads 75 kg. What is the elevator's acceleration?
    solution

    Change the scale reading back into the normal force.

    $$F_N = (75)(9.8)$$ $$F_N = 735\,\mathrm{N}$$
    $$F_g = mg$$ $$F_g = (70)(9.8)$$ $$F_g = 686\,\mathrm{N}$$

    Let up be positive.

    $$\sum F = ma$$ $$F_N - F_g = ma$$ $$735 - 686 = 70a$$ $$49 = 70a$$ $$a = 0.70\,\mathrm{\tfrac{m}{s^{2}}}$$

    The acceleration is positive, so the elevator is speeding up going up (or slowing down while going down).

    Example: A 5.0 kg shop sign hangs at rest from two vertical chains. The chains share the load equally. What is the tension in each chain?
    solution $$F_g = mg$$ $$F_g = (5.0)(9.8)$$ $$F_g = 49\,\mathrm{N}$$

    The sign isn't accelerating, so the two tensions together balance the weight.

    $$\sum F = ma$$ $$2T - 49 = 0$$ $$2T = 49$$ $$T = 24.5\,\mathrm{N}$$
    Example: A 20 kg sled is pulled across frictionless ice by a rope with 100 N of tension at 30° above the horizontal. What are the normal force and the horizontal acceleration?
    solution
    $$T_x = T\cos(30\degree)$$ $$T_x = (100)\cos(30\degree)$$ $$T_x = 86.6\,\mathrm{N}$$
    $$T_y = T\sin(30\degree)$$ $$T_y = (100)\sin(30\degree)$$ $$T_y = 50.0\,\mathrm{N}$$

    The sled doesn't accelerate vertically, so the vertical forces balance.

    $$F_N + T_y - F_g = 0$$ $$F_N + 50.0 - (20)(9.8) = 0$$ $$F_N + 50.0 - 196 = 0$$ $$F_N = 146\,\mathrm{N}$$
    $$\sum F = ma$$ $$86.6 = 20a$$ $$a = \frac{86.6}{20}$$ $$a = 4.33\,\mathrm{\tfrac{m}{s^{2}}}$$

    Pulling up at an angle lifts part of the sled's weight, so the normal force is less than 196 N.

    Example: A 30 kg cart starts from rest on a frictionless floor. A rope pulls it horizontally with 90 N for 4.0 s. What is the cart's acceleration, and how far does it move?
    solution $$\sum F = ma$$ $$90 = 30a$$ $$a = 3.0\,\mathrm{\tfrac{m}{s^{2}}}$$
    $$u = 0$$ $$a = 3.0\,\mathrm{\tfrac{m}{s^{2}}}$$ $$\Delta t = 4.0\,\mathrm{s}$$ $$\Delta x = \,?$$
    $$\Delta x = u\Delta t + \tfrac{1}{2}a\Delta t^{2}$$ $$\Delta x = (0)(4.0) + \tfrac{1}{2}(3.0)(4.0)^{2}$$ $$\Delta x = 24\,\mathrm{m}$$
    Example: A 1200 kg car moving at 72 km/h must stop in 50 m. What constant net force is needed to stop it?
    solution $$72\,\mathrm{\tfrac{\textcolor{DeepPink}{km}}{\textcolor{DodgerBlue}{h}}}\left(\frac{1000\,\mathrm{m}}{1\,\textcolor{DeepPink}{\mathrm{km}}}\right)\left(\frac{1\,\textcolor{DodgerBlue}{\mathrm{h}}}{3600\,\mathrm{s}}\right)$$ $$20\,\mathrm{\tfrac{m}{s}}$$

    Use kinematics to find the acceleration. Let forward be positive.

    $$u = 20\,\mathrm{\tfrac{m}{s}}$$ $$v = 0$$ $$\Delta x = 50\,\mathrm{m}$$ $$a = \,?$$
    $$v^{2} = u^{2} + 2a\Delta x$$ $$0^{2} = (20)^{2} + 2a(50)$$ $$0 = 400 + 100a$$ $$a = -4.0\,\mathrm{\tfrac{m}{s^{2}}}$$
    $$\sum F = ma$$ $$\sum F = (1200)(-4.0)$$ $$\sum F = -4800\,\mathrm{N}$$

    The net force is 4800 N, pointing opposite the car's motion.

    Example: A 10 kg block on a frictionless 30° ramp is connected by a rope over a pulley to a hanging 6.0 kg block. The system starts from rest, and the hanging block moves down. Find the acceleration and the tension. How long does it take the hanging block to fall 2.0 m?
    solution

    The block on the ramp is pulled back by the part of its weight that points down the ramp.

    $$F_{g\parallel} = mg\sin(30\degree)$$ $$F_{g\parallel} = (10)(9.8)\sin(30\degree)$$ $$F_{g\parallel} = 49.0\,\mathrm{N}$$
    $$F_g = (6.0)(9.8)$$ $$F_g = 58.8\,\mathrm{N}$$

    The hanging weight pulls one way and the ramp component pulls the other way.

    $$\sum F = ma$$ $$58.8 - 49.0 = (10 + 6.0)a$$ $$9.8 = 16a$$ $$a = 0.61\,\mathrm{\tfrac{m}{s^{2}}}$$

    Use the block on the ramp to find the tension.

    $$T - F_{g\parallel} = ma$$ $$T - 49.0 = (10)(0.61)$$ $$T = 55.1\,\mathrm{N}$$

    Now use kinematics for the falling block.

    $$\Delta x = u\Delta t + \tfrac{1}{2}a\Delta t^{2}$$ $$2.0 = (0)\Delta t + \tfrac{1}{2}(0.61)\Delta t^{2}$$ $$\Delta t^{2} = 6.56$$ $$\Delta t = 2.6\,\mathrm{s}$$