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Edexcel International A Level Maths: Mechanics 1

Revision Notes

Home / International A Level / Maths: Mechanics 1 / Edexcel / Revision Notes / 3. Forces & Newton’s Laws / 3.2 Newton's Second Law / 3.2.1 F = ma


3.2.1 F = ma


F = ma

What is Newton’s First Law of Motion (N1L)?

  • An object at rest will stay at rest, and an object moving with constant velocity will continue to move with constant velocity, unless an unbalanced force acts on the object
  • This law is explored more in 3.1.1 Equilibrium in 1D and 3.1.2 Equilibrium in 2D but has been included here for completeness

What is Newton’s Second Law of Motion (N2L)?

  • The resultant force (Fnet) acting on a body is equal to the product of the mass of the body and its acceleration
    • F = ma
      • F is the resultant force (N)
      • m is the mass (kg)
      • a is the acceleration (m s-2)
  • This will probably be the most familiar of Newton’s Laws of Motion as it has an equation (F = ma) that you will use frequently in mechanics problems.

What is Newton’s Third Law of Motion (N3L)?

  • For two bodies, the force exerted on the second by the first is equal in magnitude but opposite in direction to the force exerted on the first body by the second
  • This is sometimes loosely referred to as “for every action there is an opposite and equal reaction”

When do I use F= ma (Newton’s Second Law or N2L)?

  • Use it to set up and solve equations when motion is involved
  • Some related equations may come from the constant acceleration equations (‘suvat’) but F= ma is needed when force(s) and mass are mentioned or involved (neither force nor mass are involved in the ‘suvat’ equations)
  • If not asked directly in a question it will be implied by the information given – motion and acceleration will be involved and the mass of the particle will be relevant too

How do I solve problems using F= ma (N2L) and the ‘suvat’ equations?

  • F= ma can be used in conjunction with the ‘suvat’ equations – the linking connection is acceleration (a)
  • ‘suvat’ only questions will not involve mass or (resultant) force
  • Step 1. Draw a diagram and label all forces acting on the particle(s)
    • label the positive direction and any other useful information
    • If a diagram is given, add anything missing to it

  • Step 2. Use N2L, F = ma , or an appropriate ‘suvat’ equation.
    • If there is more than one particle involved you may have to do this for each

  • Step 3. Solve the equation
    • In harder problems simultaneous equations may arise.

How do we deal with forces acting in different directions on a particle in motion?

  • At AS level, if forces are acting in different directions, those directions will be perpendicular to one another
    • Thus nearly all questions at AS level involve forces acting horizontally (x-direction) and/or vertically (y-direrction)
  • In such cases we apply N2L (F = ma) and ‘suvat’ equations separately to both directions

s2kauWJB_3-2-1-fig1-forces-h-and-v

How do we use F = ma in problems involving weight?

  • Weight is a force
    • W = mg N where g m s-2 is the acceleration due to gravity
    • Weight always acts vertically downwards (towards earth)
    • If upwards is the positive direction (and assuming no other vertical forces are involved) then acceleration would be negative, a = -9.8 m s-2

    3-2-1-fig1-apple

Worked Example

3.2.1_WE_RN_F-Ma_1

(a)  Find the acceleration of the train engine.

3-2-1-fig3-we-solution-a

(b)  Find the resultant force acting on the train engine.

3-2-1-fig3-we-solution-b

(c)  Given that the (only) driving force is 6250 N, find the total of any resistive forces acting on the train engine.

3-2-1-fig3-we-solution-c

Exam Tip

  • Sketching, or adding to given, diagrams can help to understand problems and can help you decide which direction to take as positive.
  • Remember that F (in N2L) is the resultant force, sometimes seen as  Fnet- be careful not to get it muddled with any other forces that are, or could be, denoted by F.  To avoid confusion, use quote marks around “F = ma"  to show that the quoted F, m  do not necessarily correspond to a  mentioned in the question.
  • Depending on which direction is taken as positive, the resultant force, F N , may be negative and/or acceleration, a m s-2, may be negative (this is particularly relevant for vertical motion)
  • Write a list of the quantities that are given in a question and another list of those you are asked to find.  This will help you decide which equation(s) to use.
  • A third list of the quantities you are not concerned can help as these may be used to find intermediate results.


  • 1. Mechanics Toolkit
    • 1.1 Quantities, Units & Modelling
      • 1.1.1 Scalars & Vectors
        • 1.1.2 Fundamental Units
          • 1.1.3 Derived Units
            • 1.1.4 Types of Force
              • 1.1.5 Modelling Assumptions
              • 1.2 Working with Vectors
                • 1.2.1 Working with Vectors
              • 2. Kinematics (Straight Line Motion)
                • 2.1 Kinematics Graphs
                  • 2.1.1 Displacement-Time Graphs
                    • 2.1.2 Velocity-Time Graphs
                      • 2.1.3 Acceleration-Time Graphs
                        • 2.1.4 Drawing Travel Graphs
                        • 2.2 Constant Acceleration
                          • 2.2.1 Deriving the suvat Formulae
                            • 2.2.2 suvat in 1D
                              • 2.2.3 Acceleration due to Gravity
                              • 2.3 Constant Acceleration - 2D
                                • 2.3.1 suvat in 2D
                              • 3. Forces & Newton’s Laws
                                • 3.1 Forces
                                  • 3.1.1 Force Diagrams
                                    • 3.1.2 Equilibrium in 1D
                                      • 3.1.3 Equilibrium in 2D
                                        • 3.1.4 Forces in 2D - Vector Notation
                                        • 3.2 Newton's Second Law
                                          • 3.2.1 F = ma
                                            • 3.2.2 Connected Bodies - Ropes & Tow Bars
                                              • 3.2.3 Connected Bodies - The Lift Problem
                                                • 3.2.4 Connected Bodies - Pulleys
                                                  • 3.2.5 F = ma - Vector Notation
                                                  • 3.3 Further Forces & Newton's Laws
                                                    • 3.3.1 Resolving Forces & Inclined Planes
                                                      • 3.3.2 Coefficient of Friction
                                                        • 3.3.3 Coefficient of Friction - F = ma
                                                          • 3.3.4 Coefficient of Friction - Inclined Planes
                                                            • 3.3.5 Coefficient of Friction - Harder Problems
                                                            • 3.4 Momentum, Impulse & Collisions
                                                              • 3.4.1 Momentum & Impulse
                                                                • 3.4.2 Direct Collisions
                                                              • 4. Moments
                                                                • 4.1 Moments
                                                                  • 4.1.1 Moments Diagrams
                                                                    • 4.1.2 Using Moments - Equilibrium
                                                                      • 4.1.3 Centres of Mass
                                                                        • 4.1.4 Tilting


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                                                                      Author: Paul

                                                                      Paul has taught mathematics for 20 years and has been an examiner for Edexcel for over a decade. GCSE, A level, pure, mechanics, statistics, discrete – if it’s in a Maths exam, Paul will know about it. Paul is a passionate fan of clear and colourful notes with fascinating diagrams – one of the many reasons he is excited to be a member of the SME team.


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