Free-body diagrams, equilibrium and the lift · Physics Class 11–12 | StemPy Lab
Course 4.2·Lesson 2 of 3
Free-body diagrams, equilibrium and the lift
A free-body diagram shows one body alone with every force on it, and nothing else. Then the second law is applied along convenient axes. A body in equilibrium has zero net force, so the forces along each axis balance. In a lift, the scale's push is R=m(g+a)
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Try the code and the simulations beside the lesson.
A drawing that solves the problem
Almost every mistake in mechanics starts with a force left out or a force put in that is not there. The cure is a free-body diagram:
Draw the body alone, cut free from everything around it.
Draw an arrow for every force on it: weight, and one force for each thing it touches (a normal reaction, friction, a tension, a push).
Choose axes, often along and across the motion.
Apply Fnet=ma along each axis.
Watch out. Do not draw the forces the body exerts on others. There is also no "force of motion". A body moving to the right needs no force to the right, unless it is speeding up.
Equilibrium of a particle
If the net force is zero, the body is in equilibrium: at rest, or moving at a steady velocity. Then the forces balance along every axis:
ΣFx=0,ΣFy=0
A weight hangs from a knot. Two strings go from the knot up to the ceiling. The left string makes an angle of 30 degrees with the ceiling, and the right string makes an angle of 60 degrees. The tensions T one in the left string and T two in the right string pull along the strings, and the weight W pulls straight down.
For three forces in equilibrium, the arrows drawn head to tail make a closed triangle.
A person in a lift
You stand on a scale in a lift. Two forces act on you: your weight mg down, and the scale's push R up. The scale shows R. Taking up as positive:
R−mg=ma⇒R=m(g+a)
Three pictures of a person standing on the floor of a lift. When the lift accelerates up, the normal reaction N, drawn as a long arrow up, is larger than the weight m g, a shorter arrow down. When the lift moves at a steady velocity, N and m g are equal. When the lift accelerates down, N is smaller than m g.
What matters is the acceleration, not the direction of motion. Play with it.
You should find that a lift moving at a steady speed, up or down, gives your normal weight, and a lift in free fall (a=−9.8) gives zero: you feel weightless.
A worked example
A traffic light of mass 15kg hangs from two equal cables, each at 35∘to the horizontal. Find the tension.
Free-body diagram. The weight 147N down, and two tensions along the cables.
Horizontally the two horizontal parts cancel, since the cables are equal.
Vertically. Each cable lifts Tsin35∘: 2Tsin35∘=147N, so T=2×0.574147N=128N.
Think first. Each cable pulls with 128N, almost the whole weight, because flat cables have only a small upward part. A cable that is nearly horizontal needs an enormous tension.
Practise with new numbers
Try it in Python
The program follows a girl on a scale through a whole lift ride.
Remember these
Free-body diagram: one body, every force on it, nothing else.
Equilibrium: ΣFx=0 and ΣFy=0.
In a lift, R=m(g+a) with up positive: the acceleration decides, not the direction of motion.
Free fall: the scale reads zero.
Check yourself
Try each one on your own first. If you are stuck, open a hint. Then check with Show the answer.
A ball is thrown straight up. Draw (in words) its free-body diagram at the top of its path, ignoring air.
A 65kg man is in a lift that slows down while going down, at 1.5m/s2. What does the scale read? (g=9.8m/s2.)
A lamp hangs at rest from one string. What is the tension, for a 2.0kg lamp?
Why can a nearly horizontal washing line snap under a light shirt?
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