Work Formula Calculator

Work done by a force, W = Fd cos θ, with AI-powered step-by-step solutions
Find the work done by a 50 N force pushing a box 3 m
A 200 N force acts at 30 degrees to a 10 m displacement. Find the work done.
How much work is needed to lift a 15 kg box 2 m at constant speed?
Find the net work on a 4 kg block pushed with 20 N against 8 N of friction over 5 m

What Work Means in Physics

Work is energy transferred by a force acting through a displacement:

W=FdcosθW = Fd\cos\theta

Symbols and SI units:

  • WW — work, joules (J), where 1 J=1 N\cdotpm1\ \text{J} = 1\ \text{N·m}
  • FF — magnitude of the constant force, newtons (N)
  • dd — magnitude of the displacement, metres (m)
  • θ\theta — angle between the force and the displacement, degrees or radians

When the force is along the displacement, cos0°=1\cos 0° = 1 and the formula collapses to W=FdW = Fd. When the force is perpendicular, cos90°=0\cos 90° = 0 and the work is zero — which is why carrying a suitcase horizontally does no work against gravity.

The assumption people forget: W=FdcosθW = Fd\cos\theta requires a constant force along a straight path. For a varying force, work is the integral W=FdsW = \int \vec{F} \cdot d\vec{s}.

Sign, Net Work and the Work-Energy Theorem

Work is a signed scalar, not a vector:

  • 0°θ<90°0° \le \theta < 90°: positive work, energy is added to the object
  • θ=90°\theta = 90°: zero work
  • 90°<θ180°90° < \theta \le 180°: negative work, energy is removed (friction, braking)

Net work is the sum over every force acting, or equivalently Wnet=FnetdcosθW_{\text{net}} = F_{\text{net}}d\cos\theta. It links directly to kinetic energy:

Wnet=ΔKE=12mvf212mvi2W_{\text{net}} = \Delta KE = \tfrac{1}{2}mv_f^2 - \tfrac{1}{2}mv_i^2

with mm in kilograms and vv in m/s.

Lifting at constant speed: the applied force equals the weight mgmg, so W=mghW = mgh in joules, and gravity does mgh-mgh, giving zero net work and no change in speed.

The assumption people forget: an object can be under a large force and still have zero work done on it — a wall pushed hard but not moved receives no work at all.

Units check: a newton times a metre is a joule, so an answer left in N·m is already in the right unit and needs no conversion.

Common Mistakes to Avoid

  • Using force times distance travelled — the formula needs displacement, and only the component of force along it.
  • Omitting cosθ\cos\theta — an angled push does less work than its full magnitude suggests.
  • Treating work as a vector — it is a scalar with a sign, so works from several forces simply add.
  • Forgetting gg in lifting problems — to lift 1515 kg you must supply mg=147mg = 147 N, not 1515 N.
  • Confusing work with power — power is work per unit time, P=W/tP = W/t, in watts.
  • Reporting the wrong unit — the joule, not the newton. A newton-metre used as torque is a different quantity despite the identical dimensions.
  • Double-counting a force — either sum the work done by each force separately, or use the net force once, never both.
  • Thinking a curved path invalidates the formula — it does not, as long as the force magnitude and the angle to the path stay constant; otherwise integrate along the path.

示例题目

Step 1: Force and displacement are parallel, so θ=0°\theta = 0° and cosθ=1\cos\theta = 1
Step 2: W=Fdcosθ=(50 N)(3.0 m)(1)W = Fd\cos\theta = (50\ \text{N})(3.0\ \text{m})(1)
Step 3: W=150 N\cdotpm=150 JW = 150\ \text{N·m} = 150\ \text{J}
Answer: W=150W = 150 J

Step 1: W=FdcosθW = Fd\cos\theta with θ=30°\theta = 30°, so cos30°=0.8660\cos 30° = 0.8660
Step 2: Fd=(200 N)(10 m)=2000 N\cdotpmFd = (200\ \text{N})(10\ \text{m}) = 2000\ \text{N·m}
Step 3: W=(2000 N\cdotpm)(0.8660)=1732 JW = (2000\ \text{N·m})(0.8660) = 1732\ \text{J}
Step 4: The vertical component of the rope force does no work, since there is no vertical displacement
Answer: W1.73×103W \approx 1.73 \times 10^3 J

Step 1: At constant speed the applied force balances the weight: F=mgF = mg
Step 2: F=(15 kg)(9.81 m/s2)=147.2 NF = (15\ \text{kg})(9.81\ \text{m/s}^2) = 147.2\ \text{N}
Step 3: The force is upward and the displacement is upward, so θ=0°\theta = 0°
Step 4: W=Fd=(147.2 N)(2.0 m)=294 JW = Fd = (147.2\ \text{N})(2.0\ \text{m}) = 294\ \text{J}
Step 5: Gravity does 294 J-294\ \text{J} over the same lift, so the net work is zero and the speed is unchanged
Answer: W294W \approx 294 J by the lifter

常见问题

W = Fd cos θ, where F is the constant force in newtons, d is the displacement in metres, and θ is the angle between them. The answer is in joules. When the force acts along the displacement the cosine is 1 and the equation reduces to W = Fd.

Yes. When the force opposes the displacement the angle exceeds 90°, the cosine is negative, and the work is negative — meaning energy is taken out of the object. Friction and braking forces always do negative work on a moving body.

The force you apply is vertical (supporting the weight) while the displacement is horizontal, so θ = 90° and cos θ = 0. Physics work requires a displacement component along the force, which is why this feels tiring but registers as zero work.

Work is the total energy transferred, measured in joules. Power is how fast that transfer happens, P = W/t, measured in watts (joules per second). Doing 600 J in 2 s and in 10 s is the same work but 300 W versus 60 W of power.

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