physics. session kinematics - 2 session opener rest ! or motion

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Page 1: Physics. Session Kinematics - 2 Session Opener REST ! or MOTION

Physics

Page 2: Physics. Session Kinematics - 2 Session Opener REST ! or MOTION

Session

Kinematics - 2

Page 3: Physics. Session Kinematics - 2 Session Opener REST ! or MOTION

Session Opener

REST !or

MOTION

Page 4: Physics. Session Kinematics - 2 Session Opener REST ! or MOTION

Session Objectives

Page 5: Physics. Session Kinematics - 2 Session Opener REST ! or MOTION

Session Objective

1. Rest and motion

2. Distance and displacement

3. Uniform and non-uniform motion

4. Velocity

5. Acceleration

6. Equations of motion

Page 6: Physics. Session Kinematics - 2 Session Opener REST ! or MOTION

Rest and Motion

Body at rest : Position constant w.r.t. fixed point as time increases

Fixed Point : Origin of a coordinate system

Y

O900

x X

r

yP (position)

(origin)

12 2 2r ox oy

oytan

ox

ox r cos

oy r sin

Page 7: Physics. Session Kinematics - 2 Session Opener REST ! or MOTION

What is motion ?Change in position of an objectwith time, with respect to a given co ordinate system.

Motion

Actual distance traveled :Curve P0P1P2P3P4.

Displacement : Straight line P0P4 directed from P0 to P4

P0(t=0)

P1(t=t1)P2(t=t2)

P3(t=t3)P4(t=t4)

x

y

Page 8: Physics. Session Kinematics - 2 Session Opener REST ! or MOTION

Distance and Displacement

1. Distance Displacement.

1

2

x

to

2. Distance = Displacement (If direction remains same.)

3.Distance is always 0 or+ve. Displacement can be +ve,0 or –ve.

4. Distance always increases with motion.

Page 9: Physics. Session Kinematics - 2 Session Opener REST ! or MOTION

Average Speed

0 1 2 3 4

4 0

actual dis tance cov eredAverage speed

time taken

Curve lengthP PP P Ptime int erval (t t )

P0(t=0)

P1(t=t1)P2(t=t2)

P3(t=t3)P4(t=t4)

x

y

Page 10: Physics. Session Kinematics - 2 Session Opener REST ! or MOTION

Courtesy:www.physicsclassroom.com

Page 11: Physics. Session Kinematics - 2 Session Opener REST ! or MOTION

Instantaneous Speed

When time is infinitesimal (=t 0), distance is infinitesimal(=s 0)

Instantaneous speed = Limt 0

st

t

s

tt

s

Po

P1

s

Speed : Scalar

Unit m/s

Dimension LT-1

Page 12: Physics. Session Kinematics - 2 Session Opener REST ! or MOTION

Average Velocity

Average velocity is defined as displacement divided by time taken.

tr

ttrr

v12

12av

Nature : vector

Dimension : [LT-1]

Unit : m/savv

Displacement and average velocity are in same direction

r

t2t1t

2r

1r

Page 13: Physics. Session Kinematics - 2 Session Opener REST ! or MOTION

Instantaneous Velocity

If t= (t2 – t1)is extremely small (t 0)

limt 0

rv

t

v is instantaneous velocity

v is a vector.

Unit of v : m/s

r

t1t

1r

2t

2r

2t

2r

Page 14: Physics. Session Kinematics - 2 Session Opener REST ! or MOTION

Uniform Motion (One dimension)

Equal displacement (x) traveled in equal time interval (t)

1 0 02 1

1 2 1

x x x xx x... v

t 0 t t t 0

v is constant.

x = x0 + vt

If x0= 0 at t = 0 , x = vt

x0 x1 x2 x3 x4 x

0 t1t2

t3 t4t

Page 15: Physics. Session Kinematics - 2 Session Opener REST ! or MOTION

Class Exercise

Page 16: Physics. Session Kinematics - 2 Session Opener REST ! or MOTION

Class Exercise - 3

Graph in the figure below shows the variation of displacement with respect to time for a particle in one-dimensional motion. Which of the following represents the velocity-time graph of the particle in motion?

0 5t10 2015

x

Options is in next slide

Page 17: Physics. Session Kinematics - 2 Session Opener REST ! or MOTION

Class Exercise - 3

0 5t10 2015

v

(a)

0 5t10 2015

v

(b)0 5

t10 2015

v

(c)0 5

t10 2015

v

(d)

Page 18: Physics. Session Kinematics - 2 Session Opener REST ! or MOTION

Solution - 3

For t = 0 to 5

dxv ( ve and cons tant)

dt

dxt 5 to 15 v ( 0)

dt

dx

t 15 to 20 v ( ve and cons tant)dt

Hence answer is (c)

Page 19: Physics. Session Kinematics - 2 Session Opener REST ! or MOTION

Class Exercise - 8

An object travels half the distance with v1, with v2 for half of the remaining time and with v3 for the remaining half of the time. If the object never reverses the direction of motion, find the average velocity during the motion.

1 2 32v v v

4

Solution :

Page 20: Physics. Session Kinematics - 2 Session Opener REST ! or MOTION

Average Acceleration

tv

ttvv

a12

12av

Change in velocity divided by the time interval during which the change occurs.

Nature : vector

unit : m/s²

Dimension: [LT-2]

ava

v

t2t1t

2v

1v

Page 21: Physics. Session Kinematics - 2 Session Opener REST ! or MOTION

Non uniform motion (constant acceleration)

Instantaneous acceleration

v(final velocity) u(initial velocity)a

t(time taken)

FFFFFFFFFFFFFFFFFFFFFFFFFFFF

t

v

v

u

t1 t2

t=t2-t1For constant acceleration

limt 0

va

t

v = u + at Equation of motion (1)

Page 22: Physics. Session Kinematics - 2 Session Opener REST ! or MOTION

Class Exercise

Page 23: Physics. Session Kinematics - 2 Session Opener REST ! or MOTION

Class Exercise - 1

Which graph represents increasing acceleration?

v

AB

C

t

(a) A (b) B (c) C (d) None of these

Page 24: Physics. Session Kinematics - 2 Session Opener REST ! or MOTION

Solution - 1

Hence answer is (b).

Increasing a Increasing slope of

v-t curve. By observation, we find that the velocity is increasing at an increasing rate. So acceleration is increasing.

dva

dt

Page 25: Physics. Session Kinematics - 2 Session Opener REST ! or MOTION

Class Exercise - 9

An object starts from rest. It accelerates at 2 m/s2 till it reaches its maximum velocity. Then it retards at 4 m/s2 and finally comes to rest. If the total time taken is 6s, find vmax and the displacement of the object.

Page 26: Physics. Session Kinematics - 2 Session Opener REST ! or MOTION

Solution - 9

O6

Vm ax

t1 t2

Vmax = 2t1

Vmax = 4t2

s = Area of triangle

t1 = 4 s, t2 = 2 s

Hence, Vmax = 8 m/s

1

s 6 8 24 m2

2 1

2

1

1 2

4t 2t

t 1t 2

t t 6

Page 27: Physics. Session Kinematics - 2 Session Opener REST ! or MOTION

Class Exercise - 2

A particle is thrown vertically upwards with velocity v. It returns to the ground in time T. Which of the following graphs correctly represents the motion?

v

T2

T

t

(a)v T

2

t

– v

(b)

v

T2

tT

(d)v

T2

t

–v

(c)

Page 28: Physics. Session Kinematics - 2 Session Opener REST ! or MOTION

Solution - 2

The acceleration is constant (= –g). So slope has to be negative throughout the motion and velocity varies between v and –v.

Hence answer is (c).

Page 29: Physics. Session Kinematics - 2 Session Opener REST ! or MOTION

Class Exercise - 5

If a particle has an initial velocity of

and an acceleration of ,

its speed after 10 s is

7 2

(a) 10 units (b) 7 units

3 i 4 j

0.4 i 0.3 j

(c) units (d) 8.5 units

Page 30: Physics. Session Kinematics - 2 Session Opener REST ! or MOTION

Solution - 5

v u at

Hence, v 3 i 4 j 0.4 i 3 j 10

7 i 7 j

Speed v 7 2 m/s

Hence answer is (c).

Page 31: Physics. Session Kinematics - 2 Session Opener REST ! or MOTION

One dimensional equations of motion

Distance s = area under v-t graph = ½ (u+v)t

But, s = vavgt Hence, vavg = (u+v)/2

t

v

v

u

t1 t2

t=t2-t1

Using equation of motion (1)

s = ut + ½ at2 Equation of motion (2)

v uAs t , equation of motion (2)

agives

2 2v u 2a.s Equation of motion (3)

Page 32: Physics. Session Kinematics - 2 Session Opener REST ! or MOTION

One dimensional equations of motion

v = u + at

v² = u² + 2as

21s ut at

2

n

2n 1S u a

2

Distance traveled in nth second

Page 33: Physics. Session Kinematics - 2 Session Opener REST ! or MOTION

Class Exercise

Page 34: Physics. Session Kinematics - 2 Session Opener REST ! or MOTION

Class Exercise - 6

A particle moves along the X-axis as x = u(t – 3) + a(t – 3)2, then

Which of the following are true?

(a) initial velocity of particle is u at t = 0

(b) acceleration of particle is a

(c) at t = 3 the particle was at origin

(d) the particle may have negative velocity

Page 35: Physics. Session Kinematics - 2 Session Opener REST ! or MOTION

Solution - 6

The observation of displacement has started at time t = 3 s, after the object has actually started. So if it represents the time for which the object has traveled and s be the displacement after the observation has started, then general form is

21s ut at

2

2compare with s u(t – 3) a(t – 3)

Acceleration 2a, initial velocity at t 3s u

Page 36: Physics. Session Kinematics - 2 Session Opener REST ! or MOTION

Class Exercise - 10The magnitude of maximum acceleration, retardation of an object is ‘a’ m/s2. What is the minimum time taken by the object to cover a displacement ‘s’ if it starts from rest and finally comes to rest?Solution :

The minimum time would be when the acceleration is at maximum and deceleration is also maximum. Half the time accelerating at a and the rest of the time deceleration at ‘a’.

1 t sHence a t s t 2 sec

2 2 a

Page 37: Physics. Session Kinematics - 2 Session Opener REST ! or MOTION

Uniform and Non-Uniform Motion

Let us see a comparison of uniform and non-uniform motion

Courtesy:www.physicsclassroom.com

Page 38: Physics. Session Kinematics - 2 Session Opener REST ! or MOTION

Class Exercise

Page 39: Physics. Session Kinematics - 2 Session Opener REST ! or MOTION

Class Exercise - 7

An object has one-dimensional motion. If V = 6t + 4t3, then

(a) what is the distance covered from t = 3 s to t = 5 s?

(b) when is the acceleration < 0 for the first time?

5

3

3

(a) (6t 4t) dt 592

dv(b) Since is never zero

dt

So acceleration is never negative.

Solution :

Page 40: Physics. Session Kinematics - 2 Session Opener REST ! or MOTION

Class Exercise - 4A particle moves in a straight line, starting from rest. The acceleration of

the particle is given by

What is the distance traveled by the particle in the time interval 0 to seconds.

21

a sintt 1

Page 41: Physics. Session Kinematics - 2 Session Opener REST ! or MOTION

Solution - 4

2

dv 1sin t

dt t 1

t t

20 0

1dv sin t dt

t 1

t

0

1v t cos t

t 1

1

v t 2 cos tt 1

[Check that v(0) = 0]

Page 42: Physics. Session Kinematics - 2 Session Opener REST ! or MOTION

Solution - 4

dx tNow v(t)

dt

dx 12 cos t

dt t 1

x

0 0

1dx 2 cos t dt

t 1

0x [2t sin t log t 1 ]

x = 2 – log( + 1)

Page 43: Physics. Session Kinematics - 2 Session Opener REST ! or MOTION

Thank you