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Integrals in Physics

Integrals in Physics. Biblical Reference An area 25,000 cubits long and 10,000 cubits wide will belong to the Levites, who serve in the temple, as their

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Integrals in Physics

Biblical Reference

An area 25,000 cubits long and 10,000 cubits wide will belong to the Levites, who serve in the temple, as their possession for towns to live in.

Ezekiel 45:5

Why do We Need Integrals?

• When things change in Physics, they create a curved graph.

– Finding the area under a curved graph is difficult using traditional methods.

• An integral calculates the area under a curve.

Vel

ocity

(m

/s)

Time (s)

v(t)

x(t)= ∫ v(t) dt

Simple Example

With a linear function, it is easy to find the area under the curve.

vtx

mss

mx 12)4)(3(

How do you find the distance traveled in 4 seconds for an object moving 3 m/s?

t1= 1s t1= 5s

v =3 m/s

v (m/s)

t(s)

Area = 12 m

Life is not Linear…• The distance

traveled during the time interval between t1 and t2 equals the shaded area under the curve

• How do you calculate this area?

t1

v(t)

t2

v(t +Dt)

v (m/s)

t(s)

Graphs that Curve• You can approximate the

area with a series of rectangles of equal width (time interval) and adding up their areas.– There is a lot of error with

this method, because there are gaps between the rectangles and the curve.

Vel

ocity

(m

/s)

Time (sec)

ttvtxAreat

*)(lim)(0

∆t ∆t∆t∆t ∆t

The Answer… an Integral• When a continuous function is summed, a

new sign is used. It is called an Integral, and the symbol looks like this:

• When you are dealing with a situation where you have to integrate realize:– You are given: the derivative– You want: the original function

• You are working backwards – finding the antiderivative.

How do you take an Integral?• Since an integral is the opposite of a

derivative the steps are:1. Raise the power.

2. Divide by the new power.

3. Add a constant.

• Why the constant?– Remember… the derivative of a constant is

nothing. So, the integral of nothing is a constant.

Cn

xdxx

nn

)1(

)1(

Sample Problem• Start at 2m at t = 0 and start moving with the

following velocity function:

• Find the position function.

526)( 2 tttv

dttttx 526)( 2

CtttCttt

tx

52)10(

5

)11(

2

)12(

6)( 23

)10()11()12(

C2 252)( 23 ttttx

Sample Problem – with LimitsAn object is moving at velocity with respect to time according to the equation v(t) = 2t. What is:

a) The displacement function?

b) The distance traveled from t = 2 s to t = 7 s?

a)

b)

dttdtvtx )2()(

2)( ttx

44927

)2()(

22

272

7

2

7

2tdttdtvtx t

t

t

t

t

t

LIMITS

45 m

8 Simple Integral Rules

Cdx0)1

Cxdx

y

55

5

Cx

dxx

xy

)10(

55

5)10(

0

0

Ckxkdx)2

8 Simple Derivative Rules

Cn

xdxx

nn

)1()3

)1(

Cxdxx

xy

65

5

3

48

8

Cxxx

dxxx

)8

2

3

3(5

)83(5

23

2

dxxfkdxxkf )()()4

dxxgdxxfdxxgxf )()())()(()5

8 Simple Derivative Rules

Cxxx

dxxxxx

3

23

8

])35()23[(

23

22

8 Simple Derivative Rules

• Why are there only 8 (i.e. Where are the product and quotient rules)?

– Product and Quotient integration require (often) very complex substitutions. It is very rare in physics that you will be taking an integral of a product or a quotient.

8 Simple Derivative Rules

Cxdxx cos][sin)6

Cxdxx sin][cos)7

Cxdxx tan][sec)8 2

How does this apply to Physics?• Besides the kinematic equations

(acceleration, velocity and displacement), there are many other applications of an area under a curve: