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How do Newton's laws and the work-energy ideas explain the motion of objects?

Newton's laws of motion, free-body diagrams and resolving forces, balanced and unbalanced forces, motion on a slope, tension, and work done, kinetic and potential energy and power.

An SQA Higher Physics answer on forces, energy and power, covering Newton's laws of motion, free-body diagrams, resolving forces on a slope, tension, work done, kinetic and gravitational potential energy, and power.

Generated by Claude Opus 4.812 min answer

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  1. What this key area is asking
  2. Newton's laws of motion
  3. Free-body diagrams and resolving on a slope
  4. Work, energy and power
  5. Examples in context
  6. Try this

What this key area is asking

The SQA wants you to apply Newton's three laws, draw free-body diagrams and resolve forces (especially on a slope), distinguish balanced from unbalanced forces, handle tension, and use the work-energy ideas: work done, kinetic energy, gravitational potential energy and power.

Newton's laws of motion

Balanced forces (zero net force) mean zero acceleration, so the object is either stationary or moving at constant velocity. Unbalanced forces mean acceleration. Recognising "constant velocity" as "balanced forces" is the key to many slope and tension problems.

Free-body diagrams and resolving on a slope

A free-body diagram shows every force acting on a single object as an arrow. To handle a slope, resolve the weight mgmg into a component along the slope and a component perpendicular to it.

The component down the slope is what tends to accelerate an object downhill; the perpendicular component is balanced by the normal reaction. If the object moves at constant velocity up a frictionless slope, the applied force or tension exactly equals mgsinθmg\sin\theta.

Work, energy and power

Work done is the energy transferred by a force. By the work-energy principle, the net work done on an object equals its change in kinetic energy. Power is the rate of transferring energy; on a vehicle moving at steady speed vv against a resistive force FF, the engine power is P=FvP = Fv.

Examples in context

A funicular railway or a ski lift must supply a tension equal to the weight component mgsinθmg\sin\theta of the cars along the slope, plus extra to accelerate; engineers size the motor from P=FvP = Fv. A lift (elevator) accelerating upward needs a cable tension greater than the weight (Tmg=maT - mg = ma), illustrating Newton's second law. A rocket rises because the downward thrust on the exhaust gases produces an equal and opposite upward force on the rocket (third law). A cyclist at steady speed develops power P=FvP = Fv to overcome air resistance and friction; doubling the speed against air drag needs far more power. Roller coasters convert gravitational potential energy mghmgh at the top of a drop into kinetic energy 12mv2\tfrac{1}{2}mv^2 at the bottom.

Try this

Q1. State Newton's second law as an equation. [1 mark]

  • Cue. F=maF = ma (unbalanced force equals mass times acceleration).

Q2. A 3.0 kg3.0\ \text{kg} object rests on a slope at 3030^{\circ}. Calculate the component of its weight acting down the slope. Take g=9.8 N kg1g = 9.8\ \text{N kg}^{-1}. [2 marks]

  • Cue. F=mgsinθ=3.0×9.8×sin30=14.7 NF_{\parallel} = mg\sin\theta = 3.0 \times 9.8 \times \sin 30^{\circ} = 14.7\ \text{N}.

Q3. A motor lifts a 50 kg50\ \text{kg} load a height of 4.0 m4.0\ \text{m} in 8.0 s8.0\ \text{s}. Calculate the power. Take g=9.8 N kg1g = 9.8\ \text{N kg}^{-1}. [3 marks]

  • Cue. Ep=mgh=50×9.8×4.0=1960 JE_p = mgh = 50 \times 9.8 \times 4.0 = 1960\ \text{J}; P=Et=19608.0=245 WP = \frac{E}{t} = \frac{1960}{8.0} = 245\ \text{W}.

Exam-style practice questions

Practice questions written in the style of SQA exam questions on this dot point, with worked answer explainers. The year tag is the paper they imitate, not the source.

SQA Higher 20195 marksA box of mass 25 kg is pulled up a frictionless slope inclined at 20 degrees to the horizontal at a constant velocity. Calculate the component of the box's weight acting down the slope, and the tension in the rope pulling it up the slope. Take g as 9.8 N per kg.
Show worked answer →

Weight component along the slope.

Relationship: F=mgsinθF_{\parallel} = mg \sin\theta.

Substitution: F=25×9.8×sin20F_{\parallel} = 25 \times 9.8 \times \sin 20^{\circ}.

Answer: F=25×9.8×0.342=84F_{\parallel} = 25 \times 9.8 \times 0.342 = 84 N.

At constant velocity the forces are balanced, so the tension equals the component of weight down the slope: T=84T = 84 N.

Markers reward resolving the weight with sinθ\sin\theta (not cosθ\cos\theta), the numerical component, and stating that balanced forces (constant velocity) make the tension equal to it.

SQA Higher 20224 marksA car of mass 1200 kg accelerates from rest to 15 m per second in 6.0 s on a level road. Calculate the average power developed by the engine, assuming all the work done goes into kinetic energy.
Show worked answer →

Kinetic energy gained. Relationship: Ek=12mv2E_k = \tfrac{1}{2}mv^2. Substitution: Ek=12×1200×152E_k = \tfrac{1}{2} \times 1200 \times 15^2. Answer: Ek=1.35×105E_k = 1.35 \times 10^5 J.

Average power: relationship P=EtP = \frac{E}{t}, substitution P=1.35×1056.0P = \frac{1.35 \times 10^5}{6.0}, answer P=2.25×104P = 2.25 \times 10^4 W (22.5 kW).

Markers reward the kinetic energy with the squared speed, dividing by time for power, and the answer with unit. A common slip is forgetting to square the velocity.

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