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Edexcel IAL - Mechanics 3- 1.1 Motion with Variable Acceleration- Study notes  - New syllabus

Edexcel IAL – Mechanics 3- 1.1 Motion with Variable Acceleration -Study notes- New syllabus

Edexcel IAL – Mechanics 3- 1.1 Motion with Variable Acceleration -Study notes -Edexcel A level Maths- per latest Syllabus.

Key Concepts:

  • 1.1 Motion with Variable Acceleration

Edexcel IAL Maths-Study Notes- All Topics

Kinematics with Variable Acceleration

In some kinematics problems, the acceleration of a particle is not constant but varies with either the displacement \( x \) or the time \( t \).

The motion is always along a straight line.

Velocity and Acceleration Relations

The following fundamental relationships are used:

Velocity: \( v = \dfrac{dx}{dt} \)

Acceleration: \( a = \dfrac{dv}{dt} = \dfrac{d^2x}{dt^2} \)

Acceleration as a Function of Time

If acceleration is given as a function of time,

\( \dfrac{dv}{dt} = f(t) \)

Integrating with respect to \( t \) gives the velocity:

\( v = \displaystyle \int f(t)\,dt \)

A further integration gives the displacement.

Acceleration as a Function of Displacement

If acceleration is given as a function of displacement,

\( a = f(x) \)

Using the chain rule, acceleration can be written as

\( a = v\dfrac{dv}{dx} \)

So the governing equation becomes

\( v\dfrac{dv}{dx} = f(x) \)

Integrating with respect to \( x \) gives an expression for \( v \) in terms of \( x \).

Alternative Forms

The syllabus also allows equations of the form:

\( \dfrac{d^2x}{dt^2} = f(x) \)

\( \dfrac{dx}{dt} = f(t) \)

These are solved using direct integration and initial conditions.

 Problem-Solving Steps

  • Identify whether acceleration depends on \( x \) or \( t \)
  • Choose the appropriate differential equation
  • Integrate and apply initial conditions

Example :

A particle moves in a straight line with acceleration \( a = 6t \,\text{m s}^{-2} \). It starts from rest at \( t = 0 \). Find its velocity at time \( t \).

▶️ Answer/Explanation

Given

\( \dfrac{dv}{dt} = 6t \)

Integrating:

\( v = 3t^2 + C \)

Using \( v = 0 \) when \( t = 0 \), \( C = 0 \).

Conclusion: The velocity is \( v = 3t^2 \,\text{m s}^{-1} \).

Example :

The acceleration of a particle is given by \( a = 4x \,\text{m s}^{-2} \). When \( x = 0 \), the speed of the particle is \( 2 \,\text{m s}^{-1} \). Find the speed when \( x = 3 \).

▶️ Answer/Explanation

Use

\( v\dfrac{dv}{dx} = 4x \)

Integrating:

\( \dfrac{1}{2}v^2 = 2x^2 + C \)

Using \( v = 2 \) when \( x = 0 \):

\( 2 = C \)

So

\( \dfrac{1}{2}v^2 = 2x^2 + 2 \)

At \( x = 3 \):

\( v^2 = 40 \Rightarrow v = \sqrt{40} \)

Conclusion: The speed is \( \sqrt{40} \,\text{m s}^{-1} \).

Example :

A particle moves so that \( \dfrac{dx}{dt} = 2t + 1 \). Given that \( x = 3 \) when \( t = 0 \), find \( x \) in terms of \( t \).

▶️ Answer/Explanation

Integrate with respect to \( t \):

\( x = t^2 + t + C \)

Using \( x = 3 \) when \( t = 0 \):

\( C = 3 \)

Conclusion: The displacement is \( x = t^2 + t + 3 \).

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