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MC · lesson 5 of 12 · 112 min

Inclined Planes, Wedges and Screws

This lesson treats the ramp, the wedge and the screw as three versions of one idea: a sloped surface that lets a smaller effort move a load over a longer path. You start with inclined-plane geometry and why the ideal ramp ratio is length divided by height, then add friction, the normal force on an incline, and the gap between ideal and actual advantage. Later sections cover wedge length and thickness, thread pitch versus lead, single-start and multi-start screws, and how handle radius and torque set the effort on a screw jack.

Video lesson: Inclined Planes, Wedges and Screws

Video transcript

0:00 Hey there, and welcome to this explainer. Today, we are going to tackle something that honestly stresses a lot of people out, but absolutely shouldn't. We're talking about mastering mechanical comprehension, specifically ramps, wedges, and screws. And the best part, we're going to do it step-by-friendly step and completely without a calculator. So whether you're a high school grad gearing up for the ASVAB, or just someone looking to make sense of everyday physics, you are definitely in the right place. Let's get to it. Here's our game plan for today. We'll start with ramps and incline planes, then move on to wedges, which are just moving incline surfaces, and screws which are basically wrapped inclined planes. After that, we'll hit work, efficiency, and safety. Finally, we'll wrap up with a multi-step worked review, and some check yourself practice questions. All right, section one, ramps and inclined planes. The entire concept really hinges on this one incredibly simple formula. Your ideal mechanical advantage, or IMA, is just the sloped length. That's L, divided by your vertical rise, or lowercase H. That is literally it.

1:03 The length you walk up, divided by the height you're lifting the thing. Just make sure both of your measurements are using the exact same units and you're golden. Let's see this in action, right? So step one, remember that formula. IMA equals L over H. Now for step two, let's say you're pushing a cart up a ramp that's six meters long, with a vertical rise of 1.5 meters. Here's a super handy mental math hack for you. 1.5 goes into three twice, right? Which means it goes into six exactly four times. So your IMA is four. Simple. For step three, if you've got an 800-Newton load, you just divide that by your mechanical advantage of four, meaning you only need 200-Newtons of ideal effort to push that beast up the ramp. See? Absolutely no calculator needed. Now let's talk about friction, because it plays a sneaky game here. Static friction is the stubborn force resisting the start of motion, while kinetic friction takes over once you're actually sliding. But here is the wild part. Friction actually switches teams depending on what you're doing. When you're raising a load uphill, friction completely opposes you.

2:06 It fights your motion and adds to the effort you have to put in. But if you're carefully lowering a heavy crate back down, friction suddenly becomes your best friend. It pushes up the ramp and actually helps you hold that load back. Wedges, our moving inclined surfaces. If you're prepping for a test, you absolutely need to lock this formula into your brain. For wedges, the ideal mechanical advantage is just the length of the wedge divided by its thickness at the wide end. That's it. Length over thickness. Let's plug some numbers in using some straightforward mental math. Step one, our formula. IMA equals length divided by thickness. For step two, picture a wedge that's 15 centimeters long and three centimeters thick at the blunt end. Well, 15 divided by three is exactly five. That's our IMA. So step three, if you give that wedge a 300 newton push, it multiplies by that advantage of five, giving you a massive 1500 newtons of spreading power. You're basically trading a longer forward push for a super intense short sideways force.

3:10 Now, there's always a tradeoff. Thin wedges, like a sharp chisel, give you a massive mechanical advantage and slide right into materials easily. But the catch, their edges are fragile and dull pretty quickly. On the flip side, thick wedges, like a wood splitting maul, have a much lower advantage. That means you've got to put a lot more muscle behind them. But they are incredibly sturdy, survive massive impacts, and pop things apart super fast. All right, on to section three, screws, which are essentially wrapped inclined planes. Okay, before we even think about calculating forces, we have to understand how a screw actually moves. Now, the biggest trap here, and people fall for this all the time, is mixing up pitch and lead. Pitch is just the distance between two adjacent threads. But the lead, that's the actual physical distance, the screw travels in one complete turn. To find the lead, you always multiply the pitch by the number of thread starts. For a basic single start screw, lead and pitch are the same. But a lot of screws actually have multiple thread paths winding around them simultaneously. Let's walk through the math for a multi-start screw so it's crystal clear.

4:16 Step one, imagine a triple start screw with a 1.5 millimeter pitch. You multiply that 1.5 pitch by the three starts, which gives you a lead of 4.5 millimeters per turn. Simple enough, right? For step two, if you crank that screw ten full turns, ten times 4.5 means your load advances exactly 45 millimeters. And this brings us to the sheer power of the screw. The formula for a screw's ideal mechanical advantage is the circumference of the circle, your hand makes as you turn the handle. That's two times pi times the radius, or R, all divided by the lead, which is that curly little L. Think about it, you're moving your hand in this giant circle just to advance the screw a tiny, tiny fraction of an inch. Because of that, a screw can easily create a mechanical advantage in the hundreds. It's pretty incredible. Work, efficiency and safety. Okay, so ideal mechanical advantage is fantastic for a perfect, frictionless world, but we live in reality. Actual mechanical advantage, or AMA, looks at the real measured forces. AMA is just your actual load divided by your actual real world effort.

5:24 And efficiency, that's just your actual advantage divided by your ideal advantage then multiplied by 100 to make it a percent. Because friction is always a factor, your AMA is literally always going to be lower than your AMA. If you are taking the ASVAB, pay very close attention to these common traps. First, machines never, ever create energy out of nowhere. A longer ramp doesn't magically reduce the total work you do. It just stretches that same amount of work over a longer distance. Second, wedges don't create force from nothing. Third, a thicker screw diameter doesn't equal more travel distance. Only the lead dictates the travel. And lastly, a huge safety warning. Never rely on a self-locking jack by itself without solid blocks, wear and vibration mean they can and absolutely do slip. Multi-step worked review. Let's tackle a ramp problem just like you'd see on test day. Step one, we have a 1200 newton crate, a 3.2 meter ramp, and a 0.8 meter rise. Let's find our AMA.

6:26 Look at the friendly math here. 3.2 over 0.8 is exactly the same ratio as 32 divided by 8, so our AMA is just 4. Because of that, in step 2, our ideal effort is 1200 divided by 4, which is 300 newtons. But let's say our actual measured effort is 375 newtons. For step 3, we find our AMA by dividing the 1200 load by the 375 actual effort, giving us 3.2. Finally, to find efficiency, we take that AMA of 3.2 and divide it by our AMA of 4. 3.2 over 4 is like 32 over 40, which easily reduces to an 80% efficiency. Total breeze, right? Now let's try a multi-step screw problem. Step one, we've got a double-start screw with a 3-millimeter pitch. 3x2 means our lead is 6 millimeters. Step two, with a 0.3 meter handle, plugging into our AMA formula gives us roughly 314. Step three, taking a massive 6,000 newton load and dividing it by 314 means we only need about 19.1 newtons of ideal effort.

7:31 And finally, step four, finding the ideal torque. We multiply the load by the lead in meters, then divide by 2 pi. Don't panic at the decimals. 6,000 x 0.006 is exactly the same as 6 x6, which is 36. 36 divided by 2 pi leaves us with about 5.73 newtons meters. See, you can absolutely conquer these scary looking physics problems right in your head. And finally, section six, check yourself practice. All right, you are ready for this. Question one, a loading ramp is 10 meters long and rises two meters. What is its ideal mechanical advantage? Go ahead and pause the explainer for a second if you want to test out your mental math. Got it? The answer is five. Why? Because our sloped length of 10 divided by our vertical rise of two perfectly equals five. Honestly, no calculator needed. Let's do one more. A steel wedge is 18 centimeters long and three centimeters thick at its wide end. What is its ideal mechanical advantage? Take a quick pause and figure it out.

8:34 And the answer is six. Why? Because length over thickness, which is 18 divided by three, is exactly six. And there you go. You've just mastered the math behind these simple machines. It really makes you wonder with just a bit of clever geometry and some handy mental math tricks. What other complex concepts you could easily outsmart today? Keep practicing those hand calculations. Stay confident and I'll see you in the next explainer.

Contents · 68 sections
  1. Learning objectives and ASVAB scope
  2. Three machines built around a slope
  3. What a machine can and cannot do
  4. Force and distance are paired quantities
  5. Inclined-plane geometry
  6. Why the ideal ramp ratio is L divided by h
  7. Calculating ideal effort on a ramp
  8. A gentle ramp has a longer path
  9. A steep ramp approaches direct lifting
  10. Ramp angle and gravitational components
  11. Normal force is not the load weight on an incline
  12. Static versus kinetic friction
  13. Effort moving a crate uphill with friction
  14. Why the same ramp differs downhill
  15. Ideal and actual advantage are different
  16. Ramp efficiency from actual and ideal advantage
  17. Input and output distances must match the path
  18. Ramp work example with losses
  19. Ramp geometry with a right triangle
  20. Mass and weight are not interchangeable
  21. Units and significant figures on a ramp
  22. Free-body diagrams reveal the necessary forces
  23. Ramps in real work settings
  24. Wedge as a moving inclined surface
  25. Wedge length and thickness
  26. Why a thin wedge still travels farther
  27. Cutting, splitting, and fastening examples
  28. Wedge angle and penetration
  29. Wedge force illustration
  30. Friction sometimes helps a wedge stay in place
  31. Wedge geometry is model dependent
  32. A screw is an inclined plane wrapped around a cylinder
  33. Thread pitch measures adjacent thread spacing
  34. Lead measures travel per complete revolution
  35. Single-start screw calculation
  36. Multi-start screw calculation
  37. Helical path distance and screw advantage
  38. Why the handle radius matters
  39. Why smaller lead can multiply force
  40. Numerical ideal screw calculation
  41. Rotational work uses torque and angle
  42. Load work during one screw revolution
  43. Solving ideal torque for an axial load
  44. Screw pitch is not thread diameter
  45. Right-hand and left-hand threads
  46. Screw jack versus fastening screw
  47. Tapered screws and threaded fasteners
  48. Efficiency in screw mechanisms
  49. Irreversibility and self-locking caution
  50. The difference between force, work, and power
  51. Input effort versus output load
  52. Choosing among the three machines
  53. Combining a ramp with a screw drive
  54. Series of simple machines and total efficiency
  55. Conservation-of-work cross-check
  56. What happens if the load does not move
  57. Ideal assumptions must be stated
  58. Safety: ramps need secure support and traction
  59. Safety: wedges and sharp edges
  60. Safety: never rely on a lifting jack alone
  61. Common misconception: long ramp is less work
  62. Common misconception: wedge creates outward force
  63. Common misconception: every screw advances one pitch
  64. Common misconception: bigger screw equals more travel
  65. Multi-step worked review: a ramp
  66. Multi-step worked review: a screw
  67. Final checklist for multiple-choice calculations
  68. Summary: force travels farther to become easier
Visual lesson

Lesson slides

15 slides
Inclined Planes, Wedges and Screws – slide 1 of 15

Learning objectives and ASVAB scope

By the end of this lesson you should be able to explain how a ramp, a wedge, and a screw let a smaller effort move a larger load by spreading the effort over a longer distance. You will compute ideal mechanical advantage , actual mechanical advantage , screw lead, torque, and efficiency, and you will recognize the safety limits that apply when these machines hold real loads.

Three machines built around a slope

A ramp is a fixed sloped surface: the load slides or rolls up it. A wedge is a slope that moves, pushed into a gap or material so its faces spread things apart. A screw is a slope wrapped in a spiral around a shaft, so turning it drives the load along the axis. All three trade a longer effort path for a smaller effort force.

What a machine can and cannot do

A simple machine can change the size of a force, its direction, or the distance over which it acts. It cannot give you more work out than you put in. In the ideal case,

in real machines friction turns part of the input into heat, so

Any claim of getting extra energy from a ramp or screw is wrong.

Force and distance are paired quantities

Work is force times the distance moved in the direction of the force,

If a machine cuts the needed force in half, the effort must move twice as far to do the same work. Force and distance always change together in opposite directions: lower force means longer travel.

Inclined-plane geometry

An inclined plane is described by three lengths: the vertical rise , the horizontal run, and the sloped length measured along the surface. The angle is measured between the ramp and the ground. The sloped length is always the longest side.

Why the ideal ramp ratio is L divided by h

Without friction, the work you do pushing along the ramp equals the work of lifting the load straight up:

Rearranging gives the ideal mechanical advantage.

Because is longer than , the ratio is greater than 1, so the effort is smaller than the load.

Inclined plane with sloped length L, vertical rise h, horizontal run and angle θ; the effort Fe pushes the load up along the slope while its weight W acts straight down; IMA = L ÷ h.

Calculating ideal effort on a ramp

A worker pushes an 800 N cart up a ramp 6 m long that rises 1.5 m. The ideal advantage is

so the ideal effort is

Check the work:

J in and

J out.

Ramp drawn to scale, 6 m long and rising 1.5 m, with an 800 N cart pushed up the slope by 200 N; IMA = 6 ÷ 1.5 = 4.

A gentle ramp has a longer path

Suppose a 600 N load must rise 1.2 m. A 2.4 m ramp needs an ideal effort of 300 N, while a 6 m ramp needs only 120 N. Both cases require 720 J of work, because

The gentle ramp feels easier per step, but you walk farther to do the same job.

Two ramps to the same scale, both rising 1.2 m for a 600 N load: a steep 2.4 m ramp needs a 300 N push and a gentle 6 m ramp needs 120 N; both take 720 J.

A steep ramp approaches direct lifting

As a ramp gets steeper, its length shrinks toward its height and approaches 1. A 1.25 m ramp rising 1.0 m has an IMA of only 1.25, so a 500 N crate needs an ideal 400 N push. At a vertical slope,

the IMA is 1 and you are simply lifting the full weight.

Ramp angle and gravitational components

On a slope at angle , the weight splits into two parts. The part pulling down along the slope is ; the part pressing into the surface is . For a 1000 N load on a 30 degree ramp, about 500 N acts along the slope and about 866 N presses into it.

1000 N load on a 30° ramp: its weight splits into about 500 N along the slope and about 866 N into the surface.

Normal force is not the load weight on an incline

The normal force is the push of the surface back on the load, at right angles to the surface. On level ground it equals the weight, but on a slope it equals , which is smaller. A 400 N box on a 20 degree incline has a normal force of about 376 N. Since friction depends on the normal force, using the full weight overstates friction.

Static versus kinetic friction

Static friction resists the start of motion; kinetic friction acts once the object slides. Static friction can rise up to , and kinetic friction is about , with usually larger. With

N
and

on level ground, it takes 250 N to break a crate loose but only 150 N to keep it sliding.

Effort moving a crate uphill with friction

A 1000 N crate slides up a 30 degree ramp at steady speed with

The slope component is about 500 N. Friction is

N

and it points downhill, opposing the motion. The needed push along the slope is about

N

well above the frictionless value.

Why the same ramp differs downhill

Friction always opposes the motion, so its direction flips when the crate moves down. Using the same 1000 N crate and 30 degree ramp, gravity pulls about 500 N downhill while friction pushes about 173 N uphill. To lower it at steady speed, a helper must hold back only about 327 N. Friction helps when lowering and hurts when raising.

Force bars along a 30° ramp for a 1000 N crate: raising needs about 673 N (gravity 500 N plus friction 173 N); lowering needs a hold-back of only about 327 N because the 173 N of friction helps.

Ideal and actual advantage are different

Ideal mechanical advantage comes from geometry alone, such as for a ramp, and assumes no friction. Actual mechanical advantage comes from measured forces.

Because real effort must also overcome friction, AMA is always less than IMA for a real ramp, wedge, or screw.

Ramp efficiency from actual and ideal advantage

Efficiency compares what you get to what the geometry promises.

A ramp 5 m long rising 1 m has IMA 5. If a 900 N load actually needs 225 N, AMA is 4 and efficiency is

Input and output distances must match the path

On a ramp, the input distance is the length traveled along the slope, because that is the direction of your push. The output distance is the vertical rise, because the job is lifting against gravity. Mixing them up, such as using horizontal run for the input, gives the wrong work and the wrong advantage.

Ramp work example with losses

A mover pushes with 250 N along a 4 m ramp to raise a 700 N dresser 1.2 m. Input work is

J

Output work is

J

Efficiency is

and the missing 160 J became heat from friction.

Ramp 4 m long rising 1.2 m with a 700 N dresser pushed up the slope by 250 N; efficiency = ?

Ramp geometry with a right triangle

The rise, run, and slope length form a right triangle, so the Pythagorean theorem links them.

A ramp rising 0.9 m over a 1.2 m run has

m

Its IMA is

Use the slope length, not the run, in the ratio.

Right-triangle ramp to scale with rise h = 0.9 m, run 1.2 m (not used) and slope length L = 1.5 m; IMA = 1.5 ÷ 0.9 ≈ 1.67.

Mass and weight are not interchangeable

Mass, in kilograms, is the amount of matter. Weight, in newtons, is the pull of gravity on it,

with

A 50 kg drum weighs about 490 N. On a ramp with IMA 4, the ideal effort is about 122.5 N, not 12.5. Convert mass to weight before using force formulas.

Units and significant figures on a ramp

Use the same length unit for and so the ratio has no units. A ramp 3.2 m long rising 80 cm should be written as 3.2 m and 0.80 m, giving IMA 4, not 0.04. Round answers to match the precision of the given data; a ratio from two-digit measurements does not justify six digits.

Free-body diagrams reveal the necessary forces

A free-body diagram draws the load as a dot or box with every force acting on it. For a crate on a ramp, show weight straight down, the normal force perpendicular to the surface, friction along the surface opposing motion, and the applied push. Tilting your axes to match the slope makes it easy to see which components must balance.

Free-body diagram, to scale, of the 1000 N crate pushed up a 30° ramp: weight W = 1000 N straight down, normal force N ≈ 866 N out of the surface, push ≈ 673 N up the slope, friction ≈ 173 N down the slope at the contact face, with dashed components W sin θ ≈ 500 N and W cos θ ≈ 866 N along the tilted axes.

Ramps in real work settings

Loading ramps on trucks, wheelchair ramps, and boat launches are all inclined planes. Accessible ramps for wheelchairs are commonly limited to a slope of about 1 unit of rise per 12 units of run, giving an IMA near 12. That gentle slope keeps the push small enough for one person, but it means the ramp must be long, often with landings to rest.

Wedge as a moving inclined surface

A wedge is an inclined plane that does the moving instead of the load. When you drive a wedge forward, its sloped faces push sideways on whatever surrounds them. A splitting maul, a doorstop, a chisel, and the tip of a nail all act this way. A small forward push over a long distance becomes a larger sideways push over a short distance.

Wedge length and thickness

For test problems, a wedge's ideal advantage is its length divided by its thickness at the wide end.

A wedge 15 cm long and 3 cm thick at the back has IMA

Long, thin wedges give large advantages; short, fat ones give small advantages.

Wedge drawn to scale, 15 cm long and 3 cm thick at the back; IMA = 15 ÷ 3 = 5.

Why a thin wedge still travels farther

To open a gap equal to its thickness, a wedge must be driven in its full length. A thin wedge opens the gap slowly, so the effort travels a long way for each bit of spreading. That long travel is exactly why the effort can be small. A thick, blunt wedge spreads quickly but needs a much harder push.

Cutting, splitting, and fastening examples

A splitting wedge is 20 cm long and 4 cm thick, so its IMA is 5. A 300 N push on it ideally produces about 1500 N of spreading force on the log. A chisel uses the same idea to cut wood, and a nail point uses it to push fibers aside so the nail can enter.

Wedge angle and penetration

The tip angle controls how a wedge behaves. A narrow angle, like a razor or a fine chisel, gives a high advantage and enters material easily, but the thin edge dulls or chips quickly. A wider angle, like an axe or splitting maul, is sturdier and pries pieces apart faster, but it needs more force to drive in.

Two wedge tips: a narrow-angle chisel (high IMA, enters easily, dulls fast) and a wide-angle splitting maul (sturdier, spreads faster, needs more force).

Wedge force illustration

Picture a hammer striking the back of a wedge with 200 N while the wedge has a length-to-thickness ratio of 6. Ideally, the faces press outward on the material with about

N in total. The input moves a long way into the crack, and the two sides of the material move apart only a short distance.

Wedge with length-to-thickness ratio 6 driven by a 200 N push into a block whose upper and lower halves are pried apart along the wedge faces, the crack closing at the tip; each half is pushed outward, total outward ≈ 200 × 6 = 1200 N.

Friction sometimes helps a wedge stay in place

Friction lowers a wedge's efficiency, but it is also why a wedge stays put. A rubber doorstop, shims under a cabinet, or a wedge holding a tool head on its handle remain wedged because friction on their faces resists sliding back out. A perfectly slippery wedge would pop out whenever the squeezing force pushed back.

Wedge geometry is model dependent

Books measure wedges slightly differently. Some use the length of a sloped face, others the straight length along the center, and some treat a double wedge as two ramps back to back. For thin wedges these give nearly the same answer. On the ASVAB, use length divided by thickness unless the question defines something else.

A screw is an inclined plane wrapped around a cylinder

Imagine cutting a long paper triangle and rolling it around a pencil: the slanted edge spirals around like a thread. A screw thread is that ramp. Each turn of the screw slides the load a short way along the spiral slope, so the load moves along the axis while your hand moves around a much longer circular path.

A long, low paper right triangle whose slanted edge is the ramp, rolled around a pencil so the slanted edge becomes a spiral thread at the same slope.

Thread pitch measures adjacent thread spacing

Pitch is the distance from one thread crest to the next, measured along the axis. A metric bolt might have a pitch of 1.5 mm. Inch fasteners often state threads per inch instead; 20 threads per inch means a pitch of

inch

Lead measures travel per complete revolution

Lead is how far the screw or nut advances along the axis in one full turn. A screw can have more than one separate thread, called starts, wound side by side.

For a single-start screw, lead equals pitch.

Single-start screw calculation

A single-start clamp screw has a pitch of 2 mm, so its lead is also 2 mm. After 15 full turns, the clamp jaw advances

mm

To advance a known distance, divide that distance by the lead: 12 mm of travel takes

turns

Multi-start screw calculation

A triple-start screw has a pitch of 1.5 mm between neighboring crests. Its lead is

mm

so each turn advances it 4.5 mm, and 10 turns move it 45 mm. Multi-start threads, used on items like some jar lids and pen caps, close quickly with fewer turns but give less force advantage.

Right-hand single-start screw with pitch 2 mm, so lead = 2 mm, beside a triple-start screw with pitch 1.5 mm and lead 3 × 1.5 = 4.5 mm; the three threads are shown in three colours.

Helical path distance and screw advantage

In one turn, the effort at a handle of radius moves around a circle of length , while the load moves one lead .

Use the same units for and . This ratio is usually large, often in the hundreds.

Right-hand screw with a handle of radius r: the hand travels a circle of 2πr each turn while the load below moves one lead ℓ along the axis; IMA = 2πr ÷ ℓ.

Why the handle radius matters

The handle radius sets how far your hand travels per turn. Doubling the radius doubles the circumference, which doubles the IMA and cuts the ideal effort in half. This is why a vise or screw jack uses a long bar instead of a small knob. The thread did not change; only the lever arm on the input side got longer.

Why smaller lead can multiply force

Lead appears in the denominator of the screw IMA, so a finer thread gives more advantage. Halving the lead doubles the IMA, because the load now rises only half as far per turn while your hand travels the same circle. The cost is time: a fine thread needs many more turns to move the load the same distance.

Numerical ideal screw calculation

A screw jack has a 0.25 m handle and a lead of 5 mm, or 0.005 m. The handle circle is

m

To raise a 10,000 N load, the ideal effort is

N at the handle end.

Rotational work uses torque and angle

Torque is a turning effect,

measured in newton-meters. When a torque turns through an angle in radians, the work done is

One full revolution is radians, so one turn delivers

This is the same work as force times the circular distance .

Load work during one screw revolution

During one turn, the axial load moves one lead, so the work done on it is . An 8000 N load on a screw with a 4 mm lead gains

J of work per revolution.

Solving ideal torque for an axial load

Setting input work equal to output work for one turn gives

For the 8000 N load and 4 mm lead,

N·m in the ideal case. Real screws need noticeably more because of thread friction.

Screw pitch is not thread diameter

Diameter is how thick the screw is; pitch is how close the threads are. They are separate measurements. A metric bolt labeled M10 x 1.5 has a 10 mm diameter and a 1.5 mm pitch. Two bolts with the same diameter can have coarse or fine threads, and only the pitch and number of starts decide how far one turn moves the bolt.

M10 × 1.5 bolt drawn to scale with its 10 mm diameter across the threads and 1.5 mm pitch along the axis, beside a bolt of the same 10 mm diameter with fine threads.

Right-hand and left-hand threads

Most screws are right-hand: turning them clockwise, viewed from the head, drives them in or tightens them. Left-hand threads work the opposite way. They are used where normal rotation could loosen a right-hand part, such as the left pedal on a bicycle, or to keep some gas fittings from being mixed up. Handedness changes direction, not advantage.

Right-hand screw with threads rising to the right and left-hand screw with threads rising to the left; turning each clockwise as seen from the head tightens the right-hand screw and loosens the left-hand one.

Screw jack versus fastening screw

A screw jack uses a screw to lift: a long handle and a small lead create a huge IMA so a person can raise a vehicle. A fastening screw or bolt uses the same thread to clamp parts together, turning modest torque into a large pulling force along the shank. The physics is the same; the goal is lifting in one case and holding in the other.

Tapered screws and threaded fasteners

A wood screw combines two machines. Its pointed, tapered tip acts as a wedge that pushes fibers apart, and its thread acts as a spiral ramp that pulls the screw in. A machine bolt has straight threads and works with a nut; tightening the nut stretches the bolt slightly, and that stretch provides the clamping force that holds the joint.

Wood screw side view, not to scale: the tapered tip is a wedge that pushes fibers apart, and the thread is a spiral ramp that pulls the screw in.

Efficiency in screw mechanisms

Screws rub a lot of thread surface, so they are often inefficient. A screw jack with IMA 300 and a measured AMA of 90 has an efficiency of

Lubrication, smoother threads, or ball-screw designs that roll instead of slide raise efficiency, but most simple threaded screws stay well below 100%.

Irreversibility and self-locking caution

Many screws are self-locking: when you let go, the load cannot spin the screw backward because thread friction is too high. Low-efficiency screws, roughly below 50%, tend to behave this way, which is handy for a jack or a vise. Do not treat this as a guarantee. Vibration, wear, or lubrication can let a screw slip, so loads still need proper locking or support.

The difference between force, work, and power

Force is a push or pull, in newtons. Work is force times distance, in joules. Power is how fast work is done, in watts, where 1 W is 1 J per second. Pushing with 200 N over 3 m does 600 J of work; doing it in 4 s takes 150 W. A ramp lowers the force but not the work, and a slower push lowers the power.

Input effort versus output load

The effort is the force you supply at the input, such as your push on a cart or your hand on a jack handle. The load is the force the machine overcomes at the output, such as the cart's weight or the car resting on the jack. Mechanical advantage is always load divided by effort, so swapping them gives an answer less than 1 for a machine meant to help.

Choosing among the three machines

Pick a ramp when you need to raise a heavy object a moderate height and have room for a long path, such as rolling a mower into a truck. Pick a wedge to split, cut, separate, or hold something in place. Pick a screw when you need very large force, fine control, or a load that stays put, as in a vise, clamp, or jack.

Combining a ramp with a screw drive

Some leveling devices use a screw to push a wedge-shaped block under a machine foot. The screw multiplies the hand force, then the sloped block multiplies it again as it lifts. Ideal advantages in series multiply. If the screw has IMA 50 and the block has a slope ratio of 4, the total ideal advantage is

Leveling device: a horizontal screw (IMA 50) pushes a wedge-shaped block with slope ratio 4 under a machine foot, which rises; total IMA = 50 × 4 = 200.

Series of simple machines and total efficiency

When machines work in series, each one loses some energy, so their efficiencies multiply.

A screw stage at 60% feeding a wedge stage at 80% gives

or 48% overall. The combination is always less efficient than its weakest part.

Conservation-of-work cross-check

After any calculation, compare work in and work out. Output work must never exceed input work. If your numbers show a ramp delivering 900 J from 750 J of input, something is wrong: perhaps a unit was skipped or the run was used instead of the slope. Ideal answers give equal work; real answers give less out than in.

What happens if the load does not move

If you push on a crate resting on a ramp and it stays still, no work is done on the crate, because its distance moved is zero. Your force still matters: static friction and your push together balance the downhill pull. A jack holding a car up is in the same situation. Work and efficiency describe motion; a held load is a question of force balance.

Ideal assumptions must be stated

Ideal answers assume no friction, rigid parts that do not bend, a weightless machine, and steady motion with no speeding up. Real problems break some of these rules, and the actual effort is then larger than the ideal one. When an answer choice says ideal or frictionless, use geometry alone. When it gives friction or efficiency, adjust the effort upward.

Safety: ramps need secure support and traction

A ramp must be rated for the load, firmly supported, and hooked or blocked so its ends cannot slip. Keep the surface dry and clean so wheels and boots grip. Never stand downhill of a heavy load moving on a ramp; if it gets away, it rolls toward you. Use wheel chocks, winches, or a second person to control heavy items.

Safety: wedges and sharp edges

Wedge tools concentrate force on a small edge, so they can cut you as easily as the material. Wear eye protection when striking wedges, since chips and fragments can fly. Check that striking heads are not cracked or mushroomed, because flattened edges can break off. Cut away from your body and keep your free hand out of the path of a chisel or blade.

Safety: never rely on a lifting jack alone

A jack is made to lift, not to hold a load while someone works underneath. Its threads or seals can slip, and the vehicle can shift off the jack head. Before reaching under a raised load, set it on rated jack stands or solid blocking on firm, level ground, chock the wheels, and check that it is stable.

Common misconception: long ramp is less work

A longer ramp makes the push easier, not the work smaller. Lifting a load to a given height always needs at least of work. Adding length only spreads that work over more distance at a lower force. With friction, a very long ramp can even take slightly more total work, since friction acts over the whole length.

Common misconception: wedge creates outward force

A wedge does not make force from nothing. It redirects your forward push into sideways pushes and enlarges them because the input moves farther than the faces spread. The work out never exceeds the work in. A wedge that spreads with 5 times your force also opens the gap only one fifth as far as you drive it.

Common misconception: every screw advances one pitch

Only a single-start screw moves one pitch per turn. A double-start screw moves two pitches, and a triple-start moves three, because lead equals pitch times starts. If a question mentions multiple starts, multiply before you calculate travel, IMA, or torque. Using pitch alone would overstate the advantage of a multi-start screw.

Common misconception: bigger screw equals more travel

A thicker screw does not automatically move farther per turn. Travel per turn equals the lead, which depends on thread spacing and starts, not on diameter. A large bolt with fine threads can advance less per turn than a small screw with coarse threads. To compare travel, compare leads; to compare effort, also compare the handle radius.

Multi-step worked review: a ramp

A 1200 N crate must rise 0.8 m using a 3.2 m ramp. IMA is

so ideal effort is 300 N. The measured effort is 375 N, so AMA is

Efficiency is

Check: input

J

output

J
and
Ramp 3.2 m long rising 0.8 m with a 1200 N crate pushed up the slope by a measured 375 N; AMA = ? and efficiency = ?

Multi-step worked review: a screw

A double-start jack screw has 3 mm pitch, so its lead is 6 mm. With a 0.3 m handle, IMA is

Lifting 6000 N needs about 19.1 N ideally. Ideal torque is

N·m. At 25% efficiency, the real effort is about 76.4 N.

Screw jack, not to scale: a right-hand double-start screw with pitch 3 mm and lead 6 mm lifts a 6000 N load, which rises; the 0.3 m handle end travels a dashed horizontal circle, turned counterclockwise as seen from above, and the effort = ? acts along that circle.

Final checklist for multiple-choice calculations

Before choosing an answer, ask: Did I convert mass to weight? Are lengths in the same unit? For a ramp, did I use slope length over height? For a screw, did I find lead from pitch and starts? Is my effort smaller than the load for a helping machine? Does work out stay at or below work in? Is AMA no greater than IMA? Eliminate choices that break these rules.

Summary: force travels farther to become easier

Ramps, wedges, and screws are all sloped surfaces that trade distance for force. Ramp IMA is , wedge IMA is length over thickness, and screw IMA is divided by the lead, where lead is pitch times starts. AMA uses measured forces, and efficiency is AMA over IMA. Friction makes real effort larger, can make screws self-locking, and never lets output work exceed input work. Always support raised loads safely.

Quick review

Ideal mechanical advantage of a ramp
: sloped length divided by vertical rise (same units). An 800 N cart on a 6 m ramp rising 1.5 m needs an ideal 200 N push.
Trap: does a longer, gentler ramp reduce the work?
No. Lifting to height h always needs at least of work. A longer ramp lowers the force but spreads the same work over more distance; friction can even add work.
Ideal mechanical advantage of a wedge
at the wide end. A 15 cm long, 3 cm thick wedge has IMA 5. Long thin wedges give more advantage; blunt ones need more force.
Screw lead from pitch and starts
: axial travel per full turn. A triple-start screw with 1.5 mm pitch advances 4.5 mm per turn. Single-start: lead equals pitch.
Ideal mechanical advantage of a screw with a handle
: handle circle 2πr divided by lead ℓ (same units). A 0.25 m handle and 5 mm lead give about 314. Longer handle or finer lead raises IMA.
Friction on a ramp: raising vs lowering a crate
Friction always opposes motion. Raising: push = . Lowering at steady speed: hold back only . Normal force on a slope is .
Why do many screw jacks hold a load when released?
Low-efficiency screws (roughly below 50%) are self-locking: thread friction keeps the load from turning the screw back. Vibration or wear can still let it slip, so use jack stands.
Efficiency of a ramp, wedge or screw
, with AMA = load / actual effort. A 5 m ramp rising 1 m (IMA 5) needing 225 N for 900 N (AMA 4) is 80% efficient.

What next?

← Previous: Pulleys and Block-and-Tackle Systems

About this lesson

On the ASVAB Mechanical Comprehension subtest, simple-machine items often hinge on one ratio or one misconception, such as believing a long ramp reduces the work done. The lesson closes with common traps, two multi-step worked reviews and a checklist for multiple-choice calculations, plus safety notes on jacks, wedges and ramp traction.

Plan on roughly 112 minutes, and feel free to split it at the wedge and screw sections. When you finish, take the 40-question lesson test to confirm the ratios and calculations stuck.

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