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Definite Integrals in Context

Sarah Miller

Sarah Miller

9 min read

Next Topic - Distance & Speed

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Study Guide Overview

This study guide covers the concepts of position, velocity, and acceleration using integrals. It explains how to determine velocity as the integral of acceleration, and displacement as the integral of velocity, both as definite and indefinite integrals. The guide includes worked examples, practice questions, and emphasizes interpreting the total change versus value at a point for both velocity and displacement.

Definition

Key Concept

Velocity is the integral of acceleration with respect to time.

v(t)=∫a(t),dtv(t) = \int a(t) , dtv(t)=∫a(t),dt

This follows because acceleration is the derivative of velocity:

ddtv(t)=a(t)\frac{d}{dt} v(t) = a(t)dtd​v(t)=a(t)

and differentiation and integration are inverse operations.

#Total Change in Velocity

The definite integral

∫t1t2a(t),dt\int_{t_1}^{t_2} a(t) , dt∫t1​t2​​a(t),dt

represents the total change in velocity between t=t1t = t_1t=t1​ and t=t2t = t_2t=t2​.

  • Acceleration is the rate of change of velocity.
  • Thus, a(t)⋅Δta(t) \cdot \Delta ta(t)⋅Δt is the change in velocity over a small time interval Δt\Delta tΔt.
  • a(t),dta(t) , dta(t),dt is the limit of this change as Δt→0\Delta t \to 0Δt→0.
  • The integral ∫t1t2a(t),dt\int_{t_1}^{t_2} a(t) , dt∫t1​t2​​a(t),dt represents the total change in velocity.
You can also think of this as the integral calculating the **area** under an acceleration-time graph. The change in velocity is equal to this area.

#Velocity at a Particular Point

To find the velocity at a particular point in time, you need to:

  1. Determine the change in velocity between times t=t1t = t_1t=t1​ and t=t2t = t_2t=t2​.
  2. Add this change to the velocity at time t=t1t = t_1t=t1​.

v(t2)=v(t1)+∫t1t2a(t),dtv(t_2) = v(t_1) + \int_{t_1}^{t_2} a(t) , dtv(t2​)=v(t1​)+∫t1​t2​​a(t),dt

#Velocity Expression over Time

To find an expression for the velocity at any point in time, you need to:

  1. Determine the change in velocity between a time t=t0t = t_0t=t0​ and any other time ttt.
  2. Add this change to the velocity at t=t0t = t_0t=t0​.

v(t)=v(t0)+∫t0ta(w),dwv(t) = v(t_0) + \int_{t_0}^{t} a(w) , dwv(t)=v(t0​)+∫t0​t​a(w),dw

www here is simply a dummy variable used for the integration.

#Indefinite Integral Approach

Alternatively, find the indefinite integral

∫a(t),dt\int a(t) , dt∫a(t),dt

This produces an expression for the velocity, including a constant of integration, +C+C+C.

  • Use information in the question about the velocity at a particular point in time to find the value of CCC.
  • This also gives you an expression describing the velocity at any point in time.
Exam Tip

Remember that ∫t1t2a(t),dt\int_{t_1}^{t_2} a(t) , dt∫t1​t2​​a(t),dt represents the total change in velocity over a period of time, not the final velocity. This is a common error!

#Worked Example

#Example 1

The acceleration of a particle for 0≤t≤600 \le t \le 600≤t≤60 seconds is given by the function a(t)=14ta(t) = \frac{1}{4}\sqrt{t}a(t)=41​t​, where a(t)a(t)a(t) is measured in meters per second squared.

(a) Find the total change in velocity of the particle between t=10t = 10t=10 and t=20t = 20t=20.

Answer:

To find the change in velocity, we can use the definite integral of the acceleration:

∫102014t,dt\int_{10}^{20} \frac{1}{4}\sqrt{t} , dt∫1020​41​t​,dt

Evaluate the integral; factoring out the constant can help:

14∫1020t1/2,dt\frac{1}{4} \int_{10}^{20} t^{1/2} , dt41​∫1020​t1/2,dt

Using the power rule for integration:

14[23t3/2]1020\frac{1}{4} \left[ \frac{2}{3} t^{3/2} \right]_{10}^{20}41​[32​t3/2]1020​

Calculate the definite integral:

14(23(20)3/2−23(10)3/2)=9.637\frac{1}{4} \left( \frac{2}{3} (20)^{3/2} - \frac{2}{3} (10)^{3/2} \right) = 9.63741​(32​(20)3/2−32​(10)3/2)=9.637

Exam Tip

Round the answer to three decimal places and state appropriate units. The question asks for a change, so you should state if it is an increase or decrease. In this case, it is an increase of 9.637 meters per second.

(b) Given that the particle has a velocity of 2 meters per second at time t=3t = 3t=3 seconds, find the velocity of the particle at t=45t = 45t=45 seconds.

Answer:

We need to find the change in velocity between t=3t = 3t=3 and t=45t = 45t=45:

∫34514t,dt\int_{3}^{45} \frac{1}{4}\sqrt{t} , dt∫345​41​t​,dt

Using the power rule for integration:

14[23t3/2]345\frac{1}{4} \left[ \frac{2}{3} t^{3/2} \right]_{3}^{45}41​[32​t3/2]345​

Calculate the definite integral:

14(23(45)3/2−23(3)3/2)=49.446\frac{1}{4} \left( \frac{2}{3} (45)^{3/2} - \frac{2}{3} (3)^{3/2} \right) = 49.44641​(32​(45)3/2−32​(3)3/2)=49.446

Add this change to the initial velocity at t=3t = 3t=3 seconds:

2+49.446=51.4462 + 49.446 = 51.4462+49.446=51.446

Exam Tip

Round the answer to three decimal places and state appropriate units. The velocity at t=45t = 45t=45 seconds is 51.446 meters per second.

#Position as an Integral

#Definition

Key Concept

Position, or displacement, is the integral of velocity with respect to time.

s(t)=∫v(t),dts(t) = \int v(t) , dts(t)=∫v(t),dt

This follows because velocity is the derivative of displacement:

ddts(t)=v(t)\frac{d}{dt} s(t) = v(t)dtd​s(t)=v(t)

and differentiation and integration are inverse operations.

#Total Change in Displacement

The definite integral

∫t1t2v(t),dt\int_{t_1}^{t_2} v(t) , dt∫t1​t2​​v(t),dt

represents the total change in displacement between t=t1t = t_1t=t1​ and t=t2t = t_2t=t2​.

  • Velocity is the rate of change of displacement.
  • Thus, v(t)⋅Δtv(t) \cdot \Delta tv(t)⋅Δt is the change in displacement over a small time interval Δt\Delta tΔt.
  • v(t),dtv(t) , dtv(t),dt is the limit of this change as Δt→0\Delta t \to 0Δt→0.
  • The integral ∫t1t2v(t),dt\int_{t_1}^{t_2} v(t) , dt∫t1​t2​​v(t),dt represents the total change in displacement.
You can also think of this as the integral calculating the **area** under a velocity-time graph. The change in displacement is equal to this area.

#Displacement at a Particular Point

To find the displacement at a particular point in time, you need to:

  1. Determine the change in displacement between times t=t1t = t_1t=t1​ and t=t2t = t_2t=t2​.
  2. Add this change to the displacement at time t=t1t = t_1t=t1​.

s(t2)=s(t1)+∫t1t2v(t),dts(t_2) = s(t_1) + \int_{t_1}^{t_2} v(t) , dts(t2​)=s(t1​)+∫t1​t2​​v(t),dt

#Displacement Expression over Time

To find an expression for the displacement at any point in time, you need to:

  1. Determine the change in displacement between a time t=t0t = t_0t=t0​ and any other time ttt.
  2. Add this change to the displacement at t=t0t = t_0t=t0​.

s(t)=s(t0)+∫t0tv(w),dws(t) = s(t_0) + \int_{t_0}^{t} v(w) , dws(t)=s(t0​)+∫t0​t​v(w),dw

www here is simply a dummy variable used for the integration.

#Indefinite Integral Approach

Alternatively, find the indefinite integral

∫v(t),dt\int v(t) , dt∫v(t),dt

This produces an expression for the displacement, including a constant of integration, +C+C+C.

  • Use information in the question about the displacement or position at a particular point in time to find the value of CCC.
  • This also gives you an expression describing the displacement at any point in time.
Exam Tip

Remember that ∫t1t2v(t),dt\int_{t_1}^{t_2} v(t) , dt∫t1​t2​​v(t),dt represents the total change in displacement over a period of time. It is not the final displacement or position. It is also not the total distance traveled. Both of these are common errors!

#Worked Example

#Example 2

A particle moves along the xxx-axis with a velocity described by the function:

v(t)=12t−120t3v(t) = 12t - \frac{1}{20} t^3v(t)=12t−201​t3 for 0≤t≤240 \le t \le 240≤t≤24

ttt is measured in seconds.

(a) Given that at time t=3t = 3t=3 seconds, the displacement of the particle is 40 feet, find the displacement of the particle at t=10t = 10t=10 seconds.

Answer:

We need to find the total change in displacement from t=3t = 3t=3 to t=10t = 10t=10, and add this to the 40 feet displacement at t=3t = 3t=3.

The total change in displacement is found by integrating the velocity:

∫310(12t−120t3),dt\int_{3}^{10} (12t - \frac{1}{20} t^3) , dt∫310​(12t−201​t3),dt

Using the power rule for integration:

[6t2−180t4]310\left[ 6t^2 - \frac{1}{80} t^4 \right]_{3}^{10}[6t2−801​t4]310​

Calculate the definite integral:

6(10)2−180(10)4−(6(3)2−180(3)4)=422.0136(10)^2 - \frac{1}{80}(10)^4 - \left( 6(3)^2 - \frac{1}{80}(3)^4 \right) = 422.0136(10)2−801​(10)4−(6(3)2−801​(3)4)=422.013

Add this to the displacement at t=3t = 3t=3:

422.013+40=462.013422.013 + 40 = 462.013422.013+40=462.013

Exam Tip

At t=10t = 10t=10 seconds, the particle will be 462.013 feet from the origin.

(b) The particle starts its motion at t=0t = 0t=0 seconds with a displacement of zero feet. Find the length of time it takes for the particle to return to the same position that it started in.

Answer:

When the particle is back in the same place it started, its displacement will be zero again.

You could think of this as being a total change of zero from the starting point.

Use this fact, and solve for an unknown upper limit, TTT:

∫0T(12t−120t3),dt=0\int_{0}^{T} (12t - \frac{1}{20} t^3) , dt = 0∫0T​(12t−201​t3),dt=0

Integrate and substitute in the limits:

[6t2−180t4]0T=0\left[ 6t^2 - \frac{1}{80} t^4 \right]_{0}^{T} = 0[6t2−801​t4]0T​=0

Factorize and solve:

6T2−180T4=06T^2 - \frac{1}{80} T^4 = 06T2−801​T4=0

T2(6−180T2)=0T^2(6 - \frac{1}{80} T^2) = 0T2(6−801​T2)=0

T2=0T^2 = 0T2=0 or 6−180T2=06 - \frac{1}{80} T^2 = 06−801​T2=0

T=0T = 0T=0 or T=480=430≈21.909T = \sqrt{480} = 4\sqrt{30} \approx 21.909T=480​=430​≈21.909

Exam Tip

T=0T = 0T=0 corresponds to the start of the motion when the displacement was also 0. Round the answer to three decimal places. It takes 21.909 seconds for the particle to return to its starting place.

#Glossary

  • Velocity: The rate of change of displacement with respect to time.
  • Acceleration: The rate of change of velocity with respect to time.
  • Displacement: The overall change in position of an object.
  • Definite Integral: An integral evaluated over a specific interval, representing the total accumulation of a quantity.
  • Indefinite Integral: An integral without specified limits, representing a family of functions and includes a constant of integration.
  • Constant of Integration: The arbitrary constant added to the function after integrating, denoted as CCC.

#Summary and Key Takeaways

  • Velocity is the integral of acceleration with respect to time.
  • The definite integral of acceleration represents the total change in velocity over a time interval.
  • To find the velocity at a specific point, add the change in velocity to the initial velocity.
  • Displacement is the integral of velocity with respect to time.
  • The definite integral of velocity represents the total change in displacement over a time interval.
  • To find the displacement at a specific point, add the change in displacement to the initial displacement.
  • Use the indefinite integral to find general expressions for velocity and displacement, and apply initial conditions to determine constants of integration.

#Practice Questions

Practice Question
  1. Given the acceleration function a(t)=2t+1a(t) = 2t + 1a(t)=2t+1, find the velocity function v(t)v(t)v(t) if the initial velocity at t=0t = 0t=0 is 3 m/s.
Practice Question
  1. A particle has a velocity function v(t)=3t2−2t+1v(t) = 3t^2 - 2t + 1v(t)=3t2−2t+1. Calculate the total change in displacement between t=1t = 1t=1 and t=4t = 4t=4.
Practice Question
  1. If a particle starts from rest and accelerates according to the function a(t)=4a(t) = 4a(t)=4, find its velocity function and its displacement function.
Practice Question
  1. The velocity of a car is given by v(t)=5t3−t2+2tv(t) = 5t^3 - t^2 + 2tv(t)=5t3−t2+2t. Determine the displacement of the car after 3 seconds if it starts from rest.
Practice Question
  1. A particle's acceleration is given by a(t)=−6ta(t) = -6ta(t)=−6t. If the initial velocity is 12 m/s, find the time when the particle comes to rest.

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Question 1 of 9

If the acceleration of a particle is given by a(t)=6ta(t) = 6ta(t)=6t, and its initial velocity at t=0t=0t=0 is 5 m/s, what is the velocity function v(t)v(t)v(t)?

v(t)=3t2v(t) = 3t^2v(t)=3t2

v(t)=6t+5v(t) = 6t + 5v(t)=6t+5

v(t)=3t2+5v(t) = 3t^2 + 5v(t)=3t2+5

v(t)=6t2+5tv(t) = 6t^2 + 5tv(t)=6t2+5t