Monday, July 16, 2018

First year physics Notes chapter 3


First Year Physics Notes: PTB Lahore
Chapter 3: Motion and Force
Topics:
3.1: Displacement
d = r2-r1
The change in the position of a body from its initial to final position is known as displacement
3.2: Velocity
The rate of change of displacement is called velocity
v = Dd/Dt
or
The rate of change of position of a body is called velocity or
v = xf - xi / tf - ti
Displacement covered by a body in unit time is called velocity
vav = d/t
vins = limDt®0 Dd/Dt
If te instantanous velocity does not change then the the body moves with constant or uniform velocity
3.3: Acceleration:
The rate of change of velocity is called acceleration
a = vf - vi / tf - ti
a = Dv/Dt
ains = limDt®0 Dv/Dt


3.4: Velocity-Time Graph
The graph between velocity on y-axis and time on x-axis is called velocity-time graph. The slope of this graph gives us average acceleration
3.5: Review of Equations of Uniformly Accelerated Motion
s = (vf + vi)/2´t
1.  vf = vi + at
2.  s = vit + ½ at2
3.  2as = vf2 - vi2
3.6: Newton’s Laws of Motion
Frames of Reference: There are two types of frames of reference
Inertial frame of Reference and Noninertial Frame of Reference
Inertial Frame: A frame of reference that is at rest or moving with constant velocity in straight line 
v = 0 or v = constant
or
A nonaccelerated frame of reference is called inertial frame
a = 0
Noninertial Frame of Reference: A frame of reference that is accelerating or rotating or both accelerating and rotating is called noninertial frame of reference
Newton’s First Law
In the absence of any unbalanced force, if a body is is at rest it will remain at rest and if it is moving then it will continue its motion with constant velocity in straight line
Newton’s 2nd Law of Motion
When an unbalanced force acts on a body the body is accelerated in the direction of applied force. The magnitude of acceleration is directly proportional to the applied force and inversely proportional to its mass
F = ma
Newton’s 3rd Law of Motion
Action and reaction are equal in magnitude but in opposite direction
F = - F
3.7: Linear Momentum P
The Quantity of motion is called momentum or
The product of  mass and velocity is called momentum
P = mv
Relation Between Momentum and 2nd Law of Motion:
We know that acceleration is equal to the rate of change of velocity
a = vf - vi / t
multiplying by mass m on both sides
ma = mvf - mvi / t
But F = ma, mvf = Pf and  mvi = Pi so
F = Pf - Pi / t
F = DP / t
Newton’s 2nd law is defined as the rate of change of linear momentum is equal to force


Impulse
Ft = DP
The force applied for a very short time is called impulse or sudden force
Law of Conservation of Linear Momentum
In the absence of any external force, linear momentum of two or more interactiong bodies of an isolated system remamains constant.
Explanation: consider two bodies of masses m1 and m2 are moving with velocities v1 and v2 before collision and after collision their velocities become v1¢ and v2¢ then by the law of conservation of momentum
Momentum before collision = momentum after collision
m1v1 + m2v2 = m1v1¢+ m2v2¢
3.8: Elastic and Inelastic Collision
Elastic Collision: The collision in which linear momentum and kinetic energy before and after collisision
m1v1 + m2v2 = m1v1¢+ m2v2¢
and
½ m1v12 +1/2 m2v22 = ½ m1v1¢2+1/2 m2v2¢2
Elastic Collision in one Dimension
We know that linear momentum and kinetic energy befoere and after collision remains same
(1)  m1v1 + m2v2 = m1v1¢+ m2v2¢
m1v1  - m1v1¢ = m2v2¢- m2v2
(2)  ½ m1v12 +1/2 m2v22 = ½ m1v1¢2+1/2 m2v2¢2
Simplifying equation (1) and (2)
(3) m1 (v1  - v1¢) = m2 (v2¢- v2)
 ½ m1 (v12 - v1¢2) = ½ m2 (v2¢2 -v22)
(4) m1 (v1 - v1¢) (v1 + v1¢) = m2 (v2¢ -v2) (v2¢ +v2)
Now dividing equation(4) by equation (3)
m1 (v1 - v1¢) (v1 + v1¢)/ m1 (v1  - v1¢) = m2 (v2¢ -v2) (v2¢ +v2)/ m2 (v2¢- v2)
(v1 + v1¢) = (v2¢ +v2)
v1 - v2 = v2¢- v1¢     taking -1 common on right side only
(5)  (v1 - v2) = - (v1¢ - v2¢) 
This equation shows that relative velocity of approach is equal to the relative velocity of recession
In order to find the values of v1¢ and v2¢, considering equation
v2¢ = v1 - v2  + v1¢  and using in equation (1)   
m1v1 + m2v2 = m1v1¢+ m2 (v1 - v2  + v1¢)
m1v1 + m2v2 = m1v1¢+ m2v1 - m2v2  + m2v1¢
m1v1¢+ m2v1 - m2v2  + m2v1¢ = m1v1 + m2v2
m1v1¢ + m2v1¢ = m1v1 + m2v2 - m2v1 + m2v2
(m1 + m2 )v1¢ = (m1 - m2 )v1 + 2m2v2
(6) v1¢ = [m1 - m2 /m1 + m2 ]v1 + [2m2 /(m1 + m2 )]v2
Similarly, we get
(7) v2¢ = [2m1 /m1 + m2 ]v1 + [m2 - m1 /(m1 + m2 )]v2


Special Cases:
Case I: when m1= m2 = m, using in (6) and (7), we get
v1¢ = v2 and
v2¢ = v1
It means both bodies exchange their velocities
Case II: when m1= m2 = m and v2 -0, using in (6) and (7), we get
v1¢ = 0 and
v2¢ = v1
Body m1 comes to rest and body m2 gains the velocity of m1
Case III: when a lighter body collides with a massive body at rest i.e.
m1<< m2 = m and v2= 0, using in (6) and (7), we get
v1¢ = - v1 and
v2¢ = 0
Case Iv: when a massive body collides with a lighter body at rest i.e.
m2<< m1 = m and v2= 0, using in (6) and (7), we get
v1¢ = v1 and
v2¢ = 2v1

3.9: Force Due To Water Flow
F = - (m/t)v = - mass per  second ´change in velocity
The reaction force dueb to newton’s third law of motion
F = - (-m/t)v = (m/t)v
3.10: Momentum and Explosive Forces
Bullet and gun system
MV¢ = -mv
V¢ = - (m/M)v
3.11: Rocket Propulsion
a = mv/Mt
a = mv/M    when t = 1 second
3.12: Projectile Motion
A body thrown at some angle q above or below the horizontal and moving freely under the action of gravity is called projectile.
Horizontal distance
x = vx ´ t
Vertical Distance
y = ½ gt2
Horizontal Component of Velocity
Horizontal component of velocity remains constant throughout the motion so
vix = vfx = vi cosq
Vertical component of velocity changes at each instant so
vfy = vi sinq - gt
Magnitude of Velocity
v = Ö (vfx)2 +(vfy)2
tanq = vfy/ vfx
Horizontal Component of Acceleration
Since horizontal component of velocity remains constant throught the motion so there is no change in velocity therefore no acceleration
ax = 0
Vertical Component of Acceleration
In downwaqrd or upward direction, component of velocity changes at each point so there exists acceleration that is acceleration due to gravity g
ay = g
Height of The Projectile
In order to find height of projectile, we consider 3rd equation of motion
2as = vf2 - vi2
At the highest point vfy = 0, viy = vi, a = - g, s = h, using in (1)
-2gh = 0 - vi2
2gh = vi2               but viy = visinq
h = vi 2sin2q/2g
Time of Flight
Time taken by the projectile from the initial to final position is called time of flight. From 2nd  equation of motion
s = vi t + ½ gt2
but s = h = 0, using in (1)
0 = visinqt -½ gt2
½ gt2 =  visinqt
t =  2visinq/g

Range of The Projectile
The maximum distance covered by the projectile along the horizontal direction is called range of the projectile. It is denoted by R
R = vix ´ t
But  vix = vicosq   and t =  2visinq/g
R = vicosq ´2visinq/g
R = 2vi 2cosqsinq/g
R = vi 2 (2cosqsinq)/g
R = vi 2 (sin2q)/g                        (2cosqsinq) =sin2q
Maximum Range:
The range in which a projectile falls at maximum distance is called maximum range
Rmax = vi 2/g                 When sin2q = sin90 or q = 45
Common Point of Fall of  Two Projectiles:
If two projectiles are projected at different angles such that the sum of their angles is 90then they will fall at the same point e.g.
30 and 6040 and 50, 10 and 80 etc.
Application To Ballistic Missile
An unpowered and unguided missile is called ballistic missile. Air friction does count for accuracy. For long distance, ballistic missile do not reach at the target due to friction of air, spin motion of earth
For long range and greater precision powered and remote control guided missiles are used.


Special Questions:
Q: What do you mean by kinematics?
Ans: The study of motion without mass or charge is called kinematics
Q: What are the equations of  kinematics?
Ans: kinematical equations do not contain mass or charge
s = (vf + vi)/2´t
 vf = vi + at
 s = vit + ½ at2
2as = vf2 - vi2
Q: What is dynamics?
Ans: The study of motion with reference to mass or charge is called dynamics
Q: Can we derive dynanamics from  kinematics ?
Ans: If we multiply kinematical equations with mass then we get dynamics
Considering first equation of motion which is kinematical
vf = vi + at
multiplying by mass m on both sides
mvf = mvi + mat
Ft  = mvf - mvi
Ft  = Pf - Pi
F  = Pf - Pi /t
The above equation is dynamical equation

Q: Displacement is defined as the change in posion. What is the cause of displacement?
Ans: The cause of displacement is time which is not mensioned in the literature. Also the formula doesn’t show the involvement of time
If we write displacement in this way then time is shown
d = vt
d = (x/t)t                 (v = x/t)
Q: What is the mathematical formula of Newton’s first law?
Ans: Mathematical Formula For Newton’s First Law of Motion
It is very strange to note that, we have mathematical formula for Newton’s second law of motion F = ma, but no formula for Newton’s first law.
Q: how will you derive 2nd law of motion from first law?
Ans: Simple Derivation of Newton’s Ist law From 2nd Law
We know the relation between force and linear momentum
F = (Pf - Pi)/tf -ti
F = DP/Dt (Rate of change of linear momentum)
As an analogy
P = m(xf - xi)/tf -ti
P = mDx/Dt   
P = mv                           {v = Dx/Dt}
Momentum of a body is equal to the rate of change of change of position of a body of mass m which is nothing but Newton’s first law
If the position is not changing then its momentum is zero means the body is at rest P = 0
Q: How to derive Newton’s First law?
Ans: Usual Derivation of of Newton’s First Law
In the absence of an unbalanced force, linear momentum of a body is directly proportional to the its velocity and inversely proportional to its mass
(1) vµ P
(2) vµ 1/m
Combining (1) and (2), we have
vµ P/m
v = k P/m
when k =1 then
v = P/m
P = mv
Linear momentum is equal to the rate of change of position of a particle of mass m
Q: What is the relation between linear momentum and kinetic energy?
Ans: The relation between momentum and kinetic energy is given by
KE = ½ mv2
KE = ½ mv.v               but P = mv
KE = ½ P.v        or
KE = P2/2m
Q:
      
SHORT QUESTIONS AND ANSWERS
3.1: What is difference between uniform and variable velocity?
Ans:
Uniform Velocity: If a body covers equal distance in equal interval of time then its velocity is called uniform velocity
Variable Velocity: If a body doesn’t covers equal distance in equal interval of time then its velocity is called variable
3.2: An objectis thrown vertically upward. Discuss the sign of acceleration due to gravity, relative to velocity, while bthe object is in air?
Ans: During upward motion velocity decreases or negative and becomes zero at the highest point and starts increasing while falling downward but acceleration due to gravity remains constant
3.3: Can the velocity of an object reverse the direction when acceleration is constant? If so, give an example
Ans: Velocity reverses its direction while an object moves in upward direction and  returns to downward direction
3.5: A man standing on the top of  a tower throws a ball straight up with initial velocity vi  and at the same time throws a second ball straight downward with the same speed. Which ball will have larger speed when it strikes the ground? Ignore air friction
Ans: Ignoring the air friction, both bodies will have the same speed while striking the ground
v = gt

3.6: Explain the circumstances in which the velocity v and acceleration of a car are (i). parallel   (ii). Anti-parallel    (iii). Perpendicular   (iv). v = 0 but a
(v).       a = 0 but v
Ans:
i. While acceleration is positive then v and a are parallel to each other
ii. When brakes are applied then v and a are anti-parallel to each other
iii. When the car is moving on a circular path then linear velocity v and centripetal acceleration are perpendicular to each other
iv. When brakes are applied at any instant, the body stops so its velocity is zero but acceleration is not zero
v. when the body moves with constant velocity then its acceleration becomes zero
3.7: Find the change in momentum for an object subjected to a given force for a given time and state law of motion in terms of momentum?
Ans:
We know that acceleration is equal to the rate of change of velocity
a = vf - vi / t
multiplying by mass m on both sides
ma = mvf - mvi / t
But F = ma, mvf = Pf and  mvi = Pi so
F = Pf - Pi / t
F = DP / t
Newton’s 2nd law is defined as the rate of change of linear momentum is equal to force
3.9: Define impulse and show that how it is related to linear momentum?
Ans: The force applied for a very short time is called impulse or the impulse is equal to the change in momentum
Ft = DP
3.10: State the law of conservation of linear momentum pointing out the importance of isolated system?
Ans: In the absence of any external force, the momentum of two or more interacting bodies of an isolated system remains constant
Momentum before collision = momentum after collision
m1v1 + m2v2 = m1v1¢+ m2v2¢
3.11: Explain the difference between elastic and inelastic collision?
Ans:
Elastic Collision: The collision in which momentum and kinetic energy before and after the collision remains same
Inelastic Collision: The  collision in which momentum before and after collision remains same kinetic energy before and after collision doesn’t remain same is called inelastic collision
3.12: Explain what is meant by projectile motion? Show that the range of projectile is maximum when projectile is thrown at an angle of 45 with the horizontal?
Ans: when a body is thrown at some angle then the body moves under the action of gravity on a parabolic path. This type of motion is called projectile motion.
The formula for range of projectile motion is
R = vi 2 (sin2q)/g
For maximum range (sin2q) must give maximum value that is equal to 45 so that it becomes sin90 = 1 that gives us
Rmax = vi 2/g
3.13: At  what point or points in its path does a projectile its minimum speed, its maximum speed?
Ans: At the highest point of projectile motion the velocity is minimum and maximum before striking the ground




NUMERICAL PROBLEMS FROM EXERCISE
3.1: Ahelicopter is ascending vertically at the rate of 19.6 ms-1. when it is at the height of 156.8 m above the ground, a stone is dropped. How long does the stone take to reach the ground ?
Data:
vi = 19.6 ms-1,          h = 156.8 m,    g = 9.8 ms-2,    t = ? vf = 0
Solution:
2gS = vf 2 - vi 2
-2 ´9.8 ´156.8 = -19.6´19.6
156.8 = 19.6t + 4.9t2
32 = 4t + t2
t2 +4t -32 = 0
t2 +8t-4t -32 = 0
 t(t +8) -4(t +8) = 0
(t +8)(t -4) = 0
t = -8 s , t =4 s
t = 4s
3.3: A proton moving with the speed of  1.0´ 107 ms-1 passes through a 0.020 cm thick sheet of paper and emerge with a speed of  2.0´ 106 ms-1. Assuming uniform deceleration, find retardation and time taken to pass through the paper?
Data:
Vi = 1.0´ 107 ms-1,     s = 2.0´ 10-4m,     vf = 2.0´ 106 ms-1
a = ?,          t = ?
Solution:
2aS = vf 2 - vi 2
a =  vf 2 - vi 2/2s
a =  [(2.0´ 106 )2 - (1.0´ 107 )2 / 2 ´2.0´ 10-4 ]ms-2
a =  [4.0´ 10 12 - 1.0´ 1014 / 4´ 10-4 ]ms-2
a =  [10 12 (4 - 100) / 4´ 10-4 ]ms-2
a =  10 16 ´ - 96 / 4 ]ms-2
a = - 2.4´ 10 17ms-2
t = vf  - vi/a
t = 2.0´ 106  - 1.0´ 107/- 2.4´ 10 17
t = 106 (2 - 10)/- 2.4´ 10 17
t = - 8´106 /- 2.4´ 10 17
t = 3.33 ´10- 11 sec

3.4: Two masses m1 and m2 are initially at rest with a spring compressed between them. What is the ratio of the magnitudes of their velocities after the spring has been released?
Ans:
Initially both bodies are at rest so
Initial momentum Pi = 0
After releasing the spring both bodies move in opposite direction so
Final momentum Pf = - m1v1 + m2v2
By the law of conservation of momentum
Pi = Pf
0 = - m1v1 + m2v2
m1v1 = m2v2
v1 /v2 = m2/ m1
3.8: A truck weighing 2500 kg travelling at 21 ms-1 collides with a stationary car weighing 1000 kg. The truck and the car move together after the impact. Calculate their common velocity?
Data:
m1 = 2500 kg,    v1 = 21 ms-1,    m2 = 1000 kg,    v2 = 0
velocity of car and truck after collision = V = ?
Solution:
By the law of conservation of momentum
m1v1 + m2v2 = m1v1¢+ m2v2¢
m1v1 + m2v2 = m1V+ m2V
m1v1 + m2v2 = (m1 + m2 )V
V = m1v1 / (m1 + m2 )
V = 2500 ´ 21/ (2500 +1000 ) ms-1
V = 2500 ´ 21/ 3500 ) ms-1
V = 15 ms-1
3.9: Two blocks of masses 2 kg and 0.5 kg are attached to the ends of a compressed spring. The elastic potential energy stored in the spring is 10 J. Find the velocities of the blocks if the spring delivers its energy to the blocks when released?
Data:
m1 = 2 kg,    v1 = ?,    m2 = 0.5kg,    v2 = ?, PE = 10 J
Solution:
Initial Momentum = Final Momentum
0 = m1v1 + m2v2
v2 = - m1 / m2v1
v2 = - 2 / 0.5v1
v2 = - 4v1
By law of conservation of energy
½ m1v12 +1/2 m2v22 = 10
m1v12 + m2v22 = 20
2v12 + ½ v22 = 20
4v12 + 16 v12 = 40
20 v12 = 40
v12 = 2
v1 = Ö2 ms-1
v2 = - 4v1 = - 4Ö2 ms-1
v2 = - 5.6 ms-1
3.10: A football is thrown upward at an angle of 30 with respect to the horizontal. To throw a 40 m pass what must be the initial speed of the ball?
Data:
q = 30,    R = 40 m,    vi = ?
Solution:
The formula of range is given by
R = vi 2 (sin2q)/g
40 = vi 2 (sin60)/9.8
vi 2  =  40 ´9.8/ sin60
vi   =  21.3 ms-1
3.11: a ball is thrown horizontally from a height of 10 m with the velocity of 21ms-1. How far off it hit the ground and with what velocity?
Data:
Height h = 10 m
vix   =  21 ms-1
viy   =  0 ms-1
Distance x = ?
Velocity v = ?
Solution:
h = viyt +1/2 gt2
10 = 0 t + ½ ´9.8´t2
4.9´t2 = 10
t2 = 10/4.9
t = 1.414 s
x = vix t
x = 21´1.414 m
x = 30 m
3.12: A bomber dropped a bomb at a height of 490 m. when the velocity along the horizontal was 300 107 kmh-1
(a) how long it was in air/
(b) At what distance from the point vertically below the bomber at the instant that bomb was dropped, did it strike the ground?
Data:
Height h =y  = 490 m
Horizontal velocity vix = 300kmh-1 = 83.3ms-1
Vertical velocity viy = 0
X = ?
t = ?
Solution:
Y = viyt + ½ gt2
490 = 0 t + ½ ´9.8t2
490 =  4.9t2
t2 = 100
t = 10 s
x = vix ´t
x = 83.3 ´10 m
x = 833 m
3.13: Find the angle of projection of a projectile  for which its maximum height and horizontal range are equal?
Data:
Angle of projection q = ?
Maximum height = horizontal range
 vi 2sin2q/2g =  vi 2sin2q/g
sin2q/2 =  2sinq cosq
sinq =  4 cosq
sinq/ cosq =  4
 tanq =  4
q = tan-1( 4)
q = 76 
3.14: prove that the angle of projection, which exceed or fall short of 45 by an equal amounts, the ranges are equal?
Data:
For Maximum range q = 45
R1 = R2 = ?
According to given condition
q1 = 45 + 15= 60                                   q2 = 45 - 15= 30
R1 =  vi 2sin2q1/g                                R2 =  vi 2sin2q2/g

R1 =  vi 2sin120/g                             R2 =  vi 2sin60/g
R1 = (0.866) vi 2/g                              R2 =  (0.866)vi 2/g
This implies
R1 = R2
3.15: A SLBM is fired from a distance of 3000 km. If the earth is considered as flat and the angle of launch is 45 with horizontal. Find the velocity with which the missile is fired and the time taken by the SLBM to hit the target
Data:
R = 3000km = 3´106 m
Angle of launch q = 45
Velocity of missile v = ?
Time taken t = ?
Solution:
R =  vi 2sin2q/g
vi 2 = gR/sin2q
vi 2 = 9.8 ´3´106/sin90
vi  = 5.42´103 ms-1
vi  = 5.42 kms-1
t =  2visinq/g
t =  2 ´5.42´103 ´sin45/9.8
t =  782 s or 13 minutes


                                     


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