LibraryDerivation and Application of v = u + at, s = ut + 1/2 at^2, v^2 = u^2 + 2as

Derivation and Application of v = u + at, s = ut + 1/2 at^2, v^2 = u^2 + 2as

Learn about Derivation and Application of v = u + at, s = ut + 1/2 at^2, v^2 = u^2 + 2as as part of JEE Physics Mastery - Mechanics and Electromagnetism

Mastering Kinematic Equations for Competitive Exams

Welcome to this module on the fundamental kinematic equations of motion. These equations are cornerstones of classical mechanics and are frequently tested in competitive exams like JEE. We will focus on the derivation and application of the three primary equations: v=u+atv = u + at, s=ut+12at2s = ut + \frac{1}{2}at^2, and v2=u2+2asv^2 = u^2 + 2as. Understanding these equations will equip you to solve a wide range of problems involving uniformly accelerated motion.

Understanding the Variables

Before we dive into derivations, let's define the key variables used in these equations. Consistency in understanding these terms is crucial for accurate problem-solving.

SymbolMeaningUnit (SI)
uuInitial Velocitym/s
vvFinal Velocitym/s
aaAcceleration (constant)m/s²
ttTime Intervals
ssDisplacementm

Derivation of $v = u + at$

This equation relates final velocity, initial velocity, acceleration, and time. It's derived directly from the definition of acceleration.

Acceleration is the rate of change of velocity.

Acceleration (aa) is defined as the change in velocity (Δv\Delta v) divided by the time interval (Δt\Delta t) over which the change occurs. Mathematically, a=ΔvΔta = \frac{\Delta v}{\Delta t}.

Let the initial velocity be uu and the final velocity be vv after a time interval tt. The change in velocity is Δv=vu\Delta v = v - u. The time interval is Δt=t\Delta t = t. Substituting these into the definition of acceleration, we get a=vuta = \frac{v - u}{t}. Rearranging this equation to solve for vv gives us at=vuat = v - u, and finally, v=u+atv = u + at.

Derivation of $s = ut + \frac{1}{2}at^2$

This equation connects displacement, initial velocity, acceleration, and time. It's derived by considering the average velocity.

Displacement is average velocity multiplied by time.

For uniformly accelerated motion, the average velocity is the mean of the initial and final velocities: vavg=u+v2v_{avg} = \frac{u+v}{2}. Displacement (ss) is then s=vavg×ts = v_{avg} \times t.

We know that s=vavg×ts = v_{avg} \times t and vavg=u+v2v_{avg} = \frac{u+v}{2}. Substituting the first kinematic equation (v=u+atv = u + at) into the average velocity formula, we get vavg=u+(u+at)2=2u+at2=u+12atv_{avg} = \frac{u + (u + at)}{2} = \frac{2u + at}{2} = u + \frac{1}{2}at. Now, substituting this average velocity into the displacement equation: s=(u+12at)×ts = (u + \frac{1}{2}at) \times t. Distributing tt, we arrive at s=ut+12at2s = ut + \frac{1}{2}at^2.

Derivation of $v^2 = u^2 + 2as$

This third equation is useful when time is not given or is not needed. It relates final velocity, initial velocity, acceleration, and displacement.

Eliminate time from the first two equations.

We can derive this equation by eliminating time (tt) from the first two kinematic equations. From v=u+atv = u + at, we can express time as t=vuat = \frac{v-u}{a}.

Substitute the expression for tt from the first equation into the second equation: s=u(vua)+12a(vua)2s = u\left(\frac{v-u}{a}\right) + \frac{1}{2}a\left(\frac{v-u}{a}\right)^2. Simplifying this expression: s=u(vu)a+12a(vu)2a2s = \frac{u(v-u)}{a} + \frac{1}{2}a\frac{(v-u)^2}{a^2}. This becomes s=uvu2a+(vu)22as = \frac{uv - u^2}{a} + \frac{(v-u)^2}{2a}. Multiplying both sides by 2a2a to clear the denominators: 2as=2(uvu2)+(vu)22as = 2(uv - u^2) + (v-u)^2. Expanding the terms: 2as=2uv2u2+v22uv+u22as = 2uv - 2u^2 + v^2 - 2uv + u^2. Combining like terms, we get 2as=v2u22as = v^2 - u^2. Rearranging for v2v^2, we have v2=u2+2asv^2 = u^2 + 2as.

Visualizing Kinematic Motion

Consider a particle starting with initial velocity uu and undergoing constant acceleration aa. The velocity-time graph for this motion is a straight line with a positive slope (if a>0a > 0). The slope of this line represents the acceleration. The area under the velocity-time graph represents the displacement. The first equation, v=u+atv = u + at, is directly represented by the relationship between the initial velocity (uu), final velocity (vv), and the slope (aa) over time (tt). The second equation, s=ut+12at2s = ut + \frac{1}{2}at^2, corresponds to the area under this graph, which can be seen as a rectangle (utut) plus a triangle (12at2\frac{1}{2}at^2). The third equation, v2=u2+2asv^2 = u^2 + 2as, can be derived by relating the change in kinetic energy to the work done by the constant force causing the acceleration, or by algebraic manipulation of the first two equations.

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Application in Problem Solving

When solving problems, identify the knowns and unknowns. Choose the kinematic equation that includes the known variables and the unknown variable you need to find. Remember to pay close attention to the signs of velocity, acceleration, and displacement, especially in problems involving motion in different directions or under gravity.

Always ensure that the acceleration is constant for these equations to be valid. If acceleration changes, calculus-based methods are required.

Which kinematic equation is most useful when the time interval is unknown?

v2=u2+2asv^2 = u^2 + 2as

What does the slope of a velocity-time graph represent?

Acceleration

What physical quantity does the area under a velocity-time graph represent?

Displacement

Learning Resources

Kinematic Equations: Derivations and Examples(documentation)

Provides clear explanations and derivations of the kinematic equations with illustrative examples.

Physics Classroom: Kinematic Equations(documentation)

A comprehensive resource detailing the kinematic equations and their applications in physics problems.

JEE Physics: Kinematics - Motion in a Straight Line(blog)

A blog post focusing on motion in a straight line, often covering kinematic equations relevant to JEE preparation.

Understanding Kinematic Equations - Physics Explained(video)

A video tutorial that visually explains the derivation and application of the kinematic equations.

Projectile Motion - JEE Physics(documentation)

While focused on projectile motion, this page often includes a review of basic kinematic equations essential for the topic.

NCERT Physics Class 11: Motion in a Straight Line(documentation)

The official textbook chapter on motion in a straight line, providing foundational knowledge and derivations.

Kinematics - Physics LibreTexts(documentation)

An extensive open-source textbook chapter covering kinematics, including detailed derivations and examples.

JEE Main 2024 Physics Syllabus(documentation)

The official syllabus for JEE Main, which confirms the importance of kinematics and related equations.

Khan Academy: Velocity and Speed(documentation)

A foundational lesson on velocity and speed, crucial for understanding the variables in kinematic equations.

Physics Stack Exchange: Derivation of Kinematic Equations(blog)

A forum discussion providing various perspectives and methods for deriving the kinematic equations.