Category: Physic Tutorials

Simplifying physics for better understanding for students to excel in ‘A level’ and UTME

  • How to solve questions on wave motion

    How to solve questions on wave motion

    How to solve questions on wave motion

    Question 1

    Given the progressive wave equation{UTME 2008}

    capture

    calculate the wavelength.
    A. 12.4m                            B. 15.7m                   C. 17.5m                                  D. 18.6m

    Solution

    using the wave equation

    capture

    compare this wave equation with the one given in the question

    K is the phase difference

    capture

    capture

    capture

    capture

    B is the correct option

    Question 2

    If a light wave has a wavelength of 500nm in air, what is the frequency of the wave?{UTME 2009}
    A. 3.0 x 1014 Hz                  B. 6.0 x 1014 Hz              C. 6.0 x 1012 Hz                   D. 2.5 x 1014 Hz
    [c = 3 x 10^8 ms-1]

    v = f

    nanometer = 10^-9 m

    3 x 10^8 = f x 500 x 10^-9

    f = 3 x 10^8 / 500 x 10^-9

    f = 6.0 x 10^14 Hz

    B is the correct option

    Question 3

    The wavelength of a wave travelling with a velocity of 420ms-1 is 42 m. What is its
    period?{UTME 2010}
    A. 1.0s          B. 0.1s         C. 0.5s            D. 1.2s

    Solution

    v = / T

    T = / v

    T = 42 / 420

    T = 0.1 s

    B is the correct option

    Question 4

    A microphone connected to the Y-plates of a cathode-ray oscilloscope (c.r.o.) is placed in front of a loudspeaker. The trace on the screen of the c.r.o. is shown below{Cambridge may/june 2016 p12}

    capture

    The time-base setting is 0.5 ms cm–1 and the Y-plate sensitivity is 0.2 mV cm–1. What is the frequency of the sound from the loudspeaker and what is the amplitude of the trace on the c.r.o.?{ Cambridge may/june 2016 p12}

    capture

    Solution

    The y-sensitivity will measure the amplitide which is on the y-axis

    The time-base setting will measure the period which is on the x-axis

    From the graph representation a full cycle occupies 6boxes

    and one box to the x-axis o.5ms

    period (T) = no of boxes x value of one box(which is 0.5 ms)

    T = 6 X o.5 = 3 ms

    Frequency(f) = 1 /T

    f = 1 / (3 x 10^-3) = 333 Hz = 330 Hz approximately

    from the graph the amplitude occupies 3 boxes i.e. maximum displacement from the rest position

    and one box to the y-axis o.2 mv

    A mplitude = no of boxes x no of one box(which is 0.2mv)

    A = 3 x 0.2mv

    A = 0.6 mv

    A is the correct option

    Question 5

    The variation with time t of the displacement y of a wave X, as it passes a point P, is shown in

    CRO wave motion

    use the diagram to determine the frequency of wave X.{ Cambridge may/june 2016 p12}

    from the graph the period is 4.0 ms

    f = 1 / T

    f = 1 / (4 x 10^-3)

    f = 250 Hz

    Recommended: Click here to read short note on wave motion

  • Wave Motion And Points On Wave For Cambridge A level And UTME

    Wave Motion And Points On Wave For Cambridge A level And UTME

    In this article, I will discuss part of wave (e.g lowest and highest point of waves) and classes of waves. A wave allows energy to be transferred from one point to another without any particle of the medium traveling between the two points.

    Classes of Waves

    Wave motion can be classified base on:

    • Mode of Propagation

    The class of waves under this are

    Mechanical wave: this requires a material medium for propagation

    Electromagnetic wave: This travels in a vacuum

    • Mode of vibration

    The class of waves under this are:

    (i) Longitudinal waves

    (ii) Transverse waves

    Diagramatic representation of waves

    sinewave1

    Points On A Wave

    points on a wave

    • Rest position – the undisturbed position of particles when they are not vibrating.
    • Peak or Crest – the highest point above the rest position.
    • Trough – the lowest point below the rest position.
    • Amplitude – the maximum displacement of a point of a wave from its rest position.
    • Period (T): it is the time taken for a particle to undergo one complete cycle of oscillation.
    • Frequency (f): it is the number of oscillations performed by a particle per unit time.
    • Wavelength (λ): it is the distance between any two successive particles that are in phase, e.g. it is the distance between 2 consecutive crests or 2 troughs.
    • Wave speed (v): The speed at which the waveform travels in the direction of the propagation of the wave.
    • Wave front: A line or surface joining points which are at the same state of oscillation, i.e. in phase, e.g. a line joining crest to crest in a wave.
    • Displacement : it is the Position of an oscillating particle from its equilibrium position.
    • Amplitude: it is the maximum magnitude of the displacement of an oscillating particle from its equilibrium position.

    To deduce V = fλ

    capture

    capture

    capture

    no of cycle = n

    time = Tn

    distance = λn

    substitute all into the velocity = distance/time

    capture

    Note

    capture

    F is the frequency and the S.I base unit is Hertz(Hz)

    T is the period and the S.I base unit is second(s)

    λ is the wavelength and the S.I base unit is meter(m)

    therefore,

    V = fλ

    Displacement-distance graph and Displacement-time graph

    wavessinusodialtimedistance

    The first graph is a displacement-distance graph. On this graph you can find wavelenght and amplitude

    The second graph is a displacement-time graph. On this graph you can find period, frquency and amplitude

    The only difference between the two graphs is what you can calculate from it.

    Phase difference: this is an amount by which one oscillation leads or lags behiod another. it measures in degree or radian.

    Phase difference between waves that are exactly out of phase is π radians or 180 degrees

    capture

    progressive wave: it is a propagation of energy as a results of vibrations of waves which move energy from one place to another.

    Intensity: it is defined as power incident per unit area. The intensity of wave generally decreases as it travels along. The two reasons for this are:

    • The wave may spread out
    • The wave may be absorbed or scattered

    As wave spread out, its amplitude decreases

    Read: Longitudinal and Transverse waves

    The unit of intensity is capture

    capture

    I is the intensity

    A is amplitude

    f is frequency

    r is the distance from the source

    Electromagnetic waves travel with the same speed in space

    the speed of electromagnetic wave is capture

    capture
    Recommended: Solved questions on wave motion

    Related Article: Short note on oscillation

    Frequently Asked Questions On Waves

    • What is the lowest point on a wave: The lowest point is the trough
    • What is the highest point on a wave – Crest
  • How To Solve Questions On Equilibrium Of Forces

    How To Solve Questions On Equilibrium Of Forces

    Question 1

    A 90cm uniform lever has a load of 30N suspended at 15cm from one of its ends. If the fulcrum is at the centre of
    gravity, the force that must be applied at its other end to keep it in horizontal equilibrium is{UME 2003 Type 9}
    A. 15N                         B. 20N                          C. 30N                                   D. 60N.

    Solution

    capture

    sum of clockwise moment = sum of anti-clockwise moment

    x * 45 = 30 * 30

    45x = 900

    x = 900 / 45

    x = 20N

    B is the correct option

    Question 2

    A 100kg box is pushed along a road with a force of 500N. If the box moves with a uniform velocity, the coefficient of
    friction between the box and the road is{UME 2004 Type S}
    A. 0.5                  B. 0.4                         C. 1.0                             D. 0.8

    solution

    F – fr = ma

    since it moves with a uniform velocity acceleration = 0

    F = fr

    F = μR

    μ is the coefficient of friction

    F is the force applied

    R is the normal reaction which is equal to the weight = mg = 100*10 = 1000N

    μ = F/R  = 500 / 1000 = 0.5

    A is the correct option

    Question 3

    A man holds a 100 N load stationary in his hand. The combined weight of the forearm and hand is
    20 N. The forearm is held horizontal, as shown{cambridge may/june 2014 p11 ques 12}

    capture

    What is the vertical force F needed in the biceps?
    A 750 N                  B 800 N                      C 850 N                                    D 900 N

    Solution

    moment of a force = force x perpendicular distance

    Sum of clockwise moment = sum of anti-clockwise moment

    the 100N load will make a clockwise direction

    the 20N combined weight of the hand and forearm will make a clockwise direction

    the force F in the biceps will make anti-clockwise direction

    F*4 = 20*10 + 100*32

    4F = 200 +3200

    4F = 3400

    f = 3400/4

    F = 850N

    C is the correct option

    Click here to read short note on forces

    Question 4

    A uniform plank AB of length 5.0 m and weight 200 N is placed across a stream, as shown below

    capture

    A man of weight 880 N stands a distance x from end A. The ground exerts a vertical force FA on the plank at end A and a vertical force FB on the plank at end B.
    As the man moves along the plank, the plank is always in equilibrium.{cambridge may/jun 2014 p21 q3}

    The man stands a distance x = 0.50 m from end A. Use the principle of moments to
    calculate the magnitude of FB.

    Solution

    sum of clockwise moment = sum of anti-clockwise moment

    taking your moment about FA

    since it is a uniform plank, the weight of the plank will be at the mid-point of the plank

    FB will make a anticlockwise direction

    the man will make an clockwise direction

    the weight of the plank will make clockwise direction

    FB*5 = 200*2.5 +880*0.5

    5FB = 500 +440

    5FB = 940

    FB = 940 / 5

    FB = 188N

    Question 5

    A block of mass 2.0 kg is released from rest on a slope. It travels 7.0 m down the slope and falls a vertical distance of 3.0 m. The block experiences a frictional force parallel to the slope of 5.0 N.{cambridge may/june 2011 p11 que15}

    inclined plane

    What is the speed of the block after falling this distance?
    A 4.9 m s–1                   B 6.6 m s–1                       C 8.6 m s–1                               D 10.1 m s–1

    Solution

    mgsinθ – fr = ma

    sinθ = opposite / hypothenus = 3 /7

    g = 9.81 ms-2

    2*9.81*3/7   –  5 = 2*a

    8.41 – 5 = 2a

    3.41 = 2a

    a = 3.41 /2

    a = 1.7 ms-2

    using

    v2 = u2 + 2as

    initially it is at rest so

    u = 0ms-1

    distance covered is 7m

    v2 = 2*1.7*7

    v2 = 23.86

    find the square root of both sides

    v = 4.9ms-1

    A is the correct option

    Read: Moment of force

  • Notes on Forces – Couple And Inclined Plane

    Notes on Forces – Couple And Inclined Plane

    Forces on Masses in Gravitational Fields: A region of space in which a mass experiences an (attractive) force due to the presence of another mass.

    capture

    The Earth’s gravitational field is represented by parallel lines on small scales on objects like balls, cars and planes e.t.c

    capture

    The parallel lines indicate a uniform gravitation field where gravitational field strenght is constant. The weight of an object is always directed towards the center of the earth.

    Newton’s law of gravitation:
    Any two point masses attract each other with a force that is proportional to each of their masses and inversely proportional to the square of the distance between them.

    capture

    This diagram represent a non uniform field. The field strenght is inversely proportional to the squares pf the distance of separation.

    capture

    Forces on Charge in Electric Fields:
    A region of space where a charge experiences an (attractive or repulsiveforce due to the presence of another charge.

    capture

    A uniform electric field is represented by parallel lines that are equally spaced in two parallel plates. The electric field strenght in a uniform electric field is constant.

    capture

    show an understanding of the origin of the upthrust acting on a body in a fluid

    Upthrust: An upward force exerted by a fluid on a submerged or floating object; arises because of the difference in pressure between the upper and lower surfaces of the object.

    Archimedes’ Principle:

    Upthrust = weight of the fluid displaced by submerged object.

    Upthrust = Vol(submerged) x ρ(fluid) x g

    ρ represents density

    Liquid has its own weight, this causes pressure on the wall on the container in which liquid is held, it also causes pressure on any object immersed in the liquid

    capture

    show a qualitative understanding of frictional forces and viscous forces including air resistance (no treatment of the coefficients of friction and viscosity is required)

    When an object lies on a table or on the ground, the table or the ground must exert an upward force, otherwise it would be accelerated by gravity. This force is known as Normal force.

    capture

    FRICTIONAL FORCES: Frictional forces are forces that act against the direction of motion

    capture

    In this case,

    resultant force = force applied – frictional force = 15 – 3 = 12 N

    For inclined plane

    free_body-svg

    Viscous forces

    i.      A force that opposes the motion of an object in a fluid

    ii.   Only exists when there is (relative) motion

    iii.  Magnitude of viscous force increases with the speed of the object

    Air resistance

    Although we often ignore it, air resistance, R, is usually significant in real life.

    R depends on:

    i.   speed (approximately proportional to v 2 )

    ii.    cross-sectional area

    iii.    air density

    iv.      other factors like shape

    R is not a constant; it increases as the speed increases and vice versa

    When any object moves through air, the air offers a frictional resistance (drag) to the motion. This causes the object to decelerate. The deceleration is not constant but depends on the velocity of the object. The faster the object the greater the resistance and deceleration. You can experience this when an apple is dropped from the top of a building. At first v = 0, so R = 0 too, and a = –g. As the apple speeds up, R increases, and his acceleration diminishes. If he falls long enough his speed will be big enough to make R as big as mg. When this happens the net force is zero because the weight of the apple equals the air resistance, so the acceleration must be zero too. At this point you have what is called terminal velocity.

    maxresdefault

    capture

    Understand that the weight of a body may be taken as acting as at a single point

    Read: Moment of force

    TYPES OF OBJECTS/BODY

    i.    Regular/uniform body

    ii.    Irregular/ non uniform bodies

    The centre of gravity of a uniform or regular object is at its geometrical centre

    capture

    Centre of gravity for irregular object

    centre of gravity of irregular body

    Turning effect of a force

    The turning effect of a force is called the moment of the force. The moment is calculated by multiplying the force by the distance from the pivot.

    The turning effect of a force depends on two things;

    i    The size of the force

    ii   The distance from the pivot (axis of rotation)

    What is a couple?

    A Couple is defined as two Forces having the same magnitude, parallel lines of action, and opposite.

    Diagram of a couple

    couple - moment of a force

    In this situation, the sum of the forces in each direction is zero. so a couple does not affect the sum of forces equations. A force couple will however tend to rotate the body it is acting on.

    Two couples will have equal moments if

    capture

    Torque

    The turning effect of a couple is known as its torque

    By multiplying the magnitude of one Force by the distance between the Forces in the Couple, the moment due to the couple can be calculated.

    Torque:

    moment of a couple= one force(N) × perpendicular   distances   between the forces(m)

    The unit is Newton metre (Nm)

    capture

    The principle of moments.

    When an object is in equilibrium the sum of the anticlockwise moments about a turning point must be equal to the sum of the clockwise moments.

    sum of anticlockwise moments = sum clockwise moments

    capture

    sum of anticlockwise moments = sum clockwise moments

    capture

    Resolution of forces

    capture

    When 3 coplanar forces acting at a point are in equilibrium, they can be represented in magnitude and direction by the adjacent sides of a triangle taken in order.

    coplanar force

    Example

    capture

    capture

    capture

    capture

    Recommended: Solved question on forces

  • Notes on Dynamics for CIE A level Physics

    This is a short note on dynamics which includes motion and conservation of linear momentum for CIE A level Physics.

    4.1 Momentum and Newton’s laws of motion

    a) understand that mass is the property of a body that resists change in motion

    Mass: is a measure of the amount of matter in a body, and is the property of a body which resists change in motion

    In kinematics, the motion of a body is independent of its mass, it is a change in its state of motion that is affected by/ depends on its mass

    b) recall the relationship F = ma and solve problems using it, appreciating that acceleration and resultant force are always in the same direction

    c) define and use linear momentum as the product of mass and velocity

    Linear momentum: of a body is defined as the product of its mass and velocity i.e. p = m v

    Momentum = Mass x velocity

    p (kgms-1) = m (kg) x v (ms-1)

    d) define and use force as rate of change of momentum

    Force: is defined as the rate of change of momentum,

    i.e.    F = [ m (v – u) ] / t = ma or F = v dm / dt
    The {one} Newton: is defined as the force needed to accelerate a mass of 1 kg by 1 m s-2.

    F=Dp/Dt

    e) state and apply each of Newton’s laws of motion
    Newton’s First Law
    Every body continues in a state of rest or uniform motion in a straight line unless a net (external) force acts on it

    When no external unbalanced(resultant) force acts on a body, its velocity remains constant.

    An external force is required to change the velocity of a body. Internal forces does not have effect on an object motion
    Object remain at rest or in a straight line motion with constant velocity, unless acted upon by external unbalanced forces.

    The external force must be unbalanced i.e, two equal opposing forces will not change a body’s velocity. The vector sum of the forces must be greater then or less than zero

    Newton’s Second Law
    The rate of change of momentum of a body is directly proportional to the net force acting on the body, and the momentum change takes place in the direction of the net force

    1. When an external, unbalanced force acts on an object, the object accelerates, in the same direction as the net force F on the object.

    The acceleration a, varies directly as the net force F, and inversely as the mass of the object, m

    a α F, for m constant.

    a α 1/m, for F constant

    Thus, Newton’s 2nd law is a special case of law1,when F = 0,a = 0, and v is constant. Note that F, a, and v, are in the same direction.

    In nature, the only situation in which there is only one force acting on a body is when it is falling through vacuum. In other cases, more than one force acts, though the directions may differ.

    Concept of inertia
    This is a fundamental property of a body that measures its reluctance to a change in its state of motion…ability of a body to resist changes in its state of motion(the reason for law 1 occurence).

    The mass of a body is a measure of the inertia of that body. The more massive a body is the more its inertia.

    Newton’s Third Law
    When object X exerts a force on object Y, object Y exerts a force of the same type that is equal in magnitude and opposite in direction on object X.

    The two forces ALWAYS act on different objects and they form an action-reaction pair.

    If they were to act on the same body, we could never have accelerated motion, because the resultant force on any body would be zero.

    The acceleration of the two objects are different if their masses are different, so that,

    F1 = – F2

    becomes,

    m1a1 = – m2a2

    The acceleration now depends on the inertia mass of the objects. Therefore, though there are equal and opposite forces, the forces may NOT be balanced, causing resultant motion/acceleration of the two bodies. This is typical of masses in a gravitational field of the earth, where the earth seems not to be accelerating and the masses accelerate

    Forces always occur in pair. The interaction between one body and another is due to the forces between them

    4.2 Non-uniform motion:

    a) describe and use the concept of weight as the effect of a gravitational field on a mass and recall that the weight of a body is equal to the product of its mass and the acceleration of free fall

    capture

    Weight = force of gravity exerted on an object (or the force on a supporting scale)

    Weight (N) = mass (kg) x g (N/kg)  g=gravitational field strength

    b) describe qualitatively the motion of bodies falling in a uniform gravitational field with air resistance

    capture1

    When any object moves through air, the air offers a frictional resistance (drag) to the motion. This causes the object to decelerate. The deceleration is not constant but depends on the velocity of the object. The faster the object the greater the resistance and deceleration. You can experience this when you run – the faster you run, the harder the air seems to blow against.

    Therefore If a body falls under gravity, air resistance opposes the fall and the downward acceleration is therefore reduced. This means that bodies falling through air take longer to fall the same distance than in vacuum

    state the principle of conservation of momentum

    When objects of a system interact, their total momentum before and after interaction are equal if no net (external) force acts on the system

    The total momentum of an isolated system is constant

       m1 u1 + m2 u2 = m1 v1 + m2 v2 if net F = 0 {for all collisions }

    NB: Total momentum DURING the interaction/collision is also conserved

    (Perfectly) elastic collision:

    Both momentum & kinetic energy of the system are conserved.

    Inelastic collision:

    Only momentum is conserved, total kinetic energy is not conserved and the particles stick together after collision (i.e. move with the same velocity)

    capture2  capture3

    In inelastic collisions, total energy is conserved but Kinetic Energy may be converted into other forms of energy such as sound and heat energy

    Recommended: Solved questions on dynamics

    Question 1

    A ball X and a ball Y are travelling along the same straight line in the same direction, as
    shown in the fig below

    capture

    Ball X has mass 400 g and horizontal velocity 0.65 m s–1.
    Ball Y has mass 600 g and horizontal velocity 0.45 m s–1.
    Ball X catches up and collides with ball Y. After the collision, X has horizontal velocity 0.41 m s–1
    and Y has horizontal velocity v, as shown below

    capture1

    Calculate
    (i) the total initial momentum of the two balls,
    (ii) the velocity v,
    (iii) the total initial kinetic energy of the two balls.
    (iv) Explain how you would check whether the collision is elastic

    (v) Use Newton’s third law to explain why, during the collision, the change in momentum of X is
    equal and opposite to the change in momentum of Y.

    Before collision, the balls are moving in the same direction, therfore,

    total momentum before collision = m1u1+ m2u2

    = 0.4*0.65 + 0.6*0.45 = 0.53kgms-1

    the total initial momentum of the two balls = 0.53kgms-1

    After collision, the balls also moved in the same direction

    total momentum after collision = m1v1+m2v2

    = 0.4*0.41 + 0.6*v

    total momentum before collision = total momentum after collision (law of conservation of linear momentum)

    0.53 = 0.16 +0.6v

    0.6v = 0.37

    v = 0.37/0.6

    v = 0.617

    iii) the total initial kinetic energy of the two balls

    1/2 m1 u1^2 +1/2 m2u2^2

    1/2 *0.4*0.65^2 +1/2 *0.6*o.45^2

    0.145 J

    iv) how you would check whether the collision is elastic

    check whether the relative speed of approach equals relative speed of separation

    or

    total final kinetic energy equals the total initial kinetic energy

    v) Use Newton’s third law to explain why, during the collision, the change in momentum of X is
    equal and opposite to the change in momentum of Y

    Newton’s Third Law
    When object X exerts a force on object Y, object Y exerts a force of the same type that is equal in magnitude and opposite in direction on object X.

    Change in momentum of x = m1(v-u) = 0.4(0.41-0.65) = -0.1kgms-1

    F = dp/dt

    Change in momentum of y = m2(v-u) = 0.6(0.617-0.45) = 0.1kgms-1

    the two balls will have the same time of impact during collision

    therefore -Fx = Fy ………. this satisfy Newton’s third law of motion

    It can be put in this way:

    the forces on the two bodies (or on X and Y) are equal and opposite
    time same for both forces and force is change in momentum / time

    Two balls X and Y are supported by long strings, as shown below

    capture

    The balls are each pulled back and pushed towards each other. When the balls collide at the
    position shown in Fig. 3.1, the strings are vertical. The balls rebound in opposite directions

    Figure below shows data for X and Y during this collision.

    capture1

    The positive direction is horizontal and to the right.
    Use the conservation of linear momentum to determine the mass M of Y.

    From the key points given

    m1u1 +m2u2  = m1v1 +m2v2

    In the question given, before coollision the objects move in opposite direction toward each other and that is the reason for the negative velocity included in the question

    therefore, total mometum before collision is

    m1u1 – m2u2 = 0.05 *4.5 – M *2.8

    note that the mass is in gramm(50g) but it has been converted to kilogramm (0.05), so that all the unit will be in S.I base unit.

    After collision, the total momentum is

    m2v2 -m2v2 = M* 1.4 – 0.05 *1.8

    from law of conservation of linear momentum

    0.05 *4.5 – M *2.8 = M* 1.4 – 0.05 *1.8

    collecting like terms

    0.225 +0.09 = 4.2M

    0.315 = 4.2M

    M = 0.315/4.2

    M = 0.075Kg 0r 75g

    A child on a sledge slides down a hill with acceleration a. The hill makes an angle θ with the
    horizontal

    capture

    The total mass of the child and the sledge is m. The acceleration of free fall is g.
    What is the friction force F ?
    A m(g cosθ – a)
    B m(g cosθ + a)
    C m(g sinθ – a)
    D m(g sinθ + a)

    According to Newton’s first law of motion

    Object remain at rest or in a straight line motion with constant velocity, unless acted upon by external unbalanced forces

    so, therefore we have two unbalanced forces acting on the boy, which are force down the slope and the frictional force.

    The body accelerate uniformly down the slope because of there is a resultant force or net force

    the net force = ma

    therefore,

    F -Fr = ma

    F is the force down the slope

    Fr is the frictional force opposing the motion of the boy

    F = mgsinθ

    mgsinθ – Fr = ma

    Fr  = mgsinθ -ma

    factorise, we then have

    Fr = m(gsinθ -a)

    the correct answer is C

  • Notes On Deformation Of Solids For Cambridge A Level

    Notes On Deformation Of Solids For Cambridge A Level

    Deformation can be referred to as change of shape. For this kind of deformation either a tensile force which is responsible for stretching or compressive force which is responsible for squashing must be applied for deformation to occur.

    Hooke’s Law

    hooke's law

    It states that provided the elastic limit is not exceeded, the extension(e) is directly proportional to the force applied

    mathematically

    F α e

    F = Ke

    F = force applied(N)

    K = force constant (Nm-1)

    e = extension(m)

    It means before a material extends there must be force applied. This implies that extension depends on the force applied.

    Extension: It is the change in length of a spring

    Load: The weight attached to the spring

    Graphicaly

    hookes-law-graph

    From this graph

    force constant(k) = inverse of the graph’s slope

    Another Hooke’s law graph

    2

    Force constant = the slope of the graph

    The two graphs represent Hooke’s law. The only difference is how to calculate the force constant from the graphs.

    Elastic limit:It is the maximum point where an elastic material can still return to its original size, shape, lenght and position if the force or load of distortion is removed.

    a-phy-matdef-dia0b

    p is the elastic limit

    Elastic deformation can be define as the change in shape/size/length/dimension when force is removed and its returns to original shape/size

    Plastic deformation it is point beyond the elastic limit where an elastic material losses its elastic properties.

    Strain energy: when an object has its shape changed by forces acting on it, the object is said to be strained. strain energy is energy stored in a body due to change of shape.

    figure_17_01_05a

    capture

    x = extension

    Arrangement of spring in series and parallel

    gambar-2

    For the second springs arranged in series

    The total extension =

    capture

    Total force constant =

    capture

    For the first springs arranged in parallel

    Total extension =

    capture

    Total force constant =

    capture

    Young’s Modulus

    It represents how easy it is to deform (stretch a material) or the measure of the stiffness of a material.

    It can be define as the ratio of Tensile stress to tensile strain provided the limit of proportionality is not exceeded.

    The Young’s modulus does not depend on the length of the wire but on the material that made the wirei.e increase on decrease in length of the wire doesn’t affect the youn modulus

    capture

    Stress is the force per unit cross-sectional area of the wire

    strain is the fractional increase in the original length of the wire

    Measurement of the Young Modulus

    young modulus experiment

    The Young’s modulus of this wire can be measured using this set up. The extension varies as the slotted masses changes. The extension can be detected as the marker on the wire changes position, and the new position being measured on the rule

    What to measured and the measurement instrument

    • initial length: A meter rule to measure the initial length
    • diameter : A micrometer screw guage to measure the diameter of the wire
    • extension: A marker and ruler to measure the extension
    • force : A spring balance

    Graphical representation of Young’s modulus

    image1

    To calculate Young’s modulus, you will find the slope of the graph i.e the slope of the graph = Young’s modulus

    Types of material

    • Brittle : Materials break at the elastic limit. Example glass
    • Ductile : Materials become permanently deformed if they stretched beyond the elastic limit i.e they show plastic behaviour. Example Copper

    Graph for brittle

    images

    Graph for ductile

    ductile_material

    Recommended: Solved questions on deformation of solids and kinematics

  • Notes on Kinematics – One Dimensional Motion and Projectile

    Notes on Kinematics – One Dimensional Motion and Projectile

    Notes on Kinematics – One Dimensional Motion and Projectile

    This note summarizes everything you need to know on kinematics in a simple way. It os brief and concise.

    Definition of terms

    Displacement: It is the distance moved in a particular direction. It is a vector quantity. The S.I unit is (m)

    Velocity: It is the rate of change of displacement. It is a vector quantity. The S.I unit is (ms-1)

    Speed : It is the rate of change of distance. It is a scalar quantity. The S.I unit is (ms-1)

    Acceleration: It is the rate of change of velocity. It is a vector quanity. The S.I unit is (ms-2)

    Uniform Speed: This is equal distance at equal time interval

    Graphical representation of Uniform Speed

    capture

    Uniform Acceleration: This is equal velocity at equal time interval

    Graphical representation of uniform acceleration

    capture1

    Mathematical Expressions

    speed = distance/ time = d / t

    velocity = displacement / time  = d / t

    Average speed : Total distance/ total time taken

    Acceleration = change of velocity / time  = (v – u) / t

    v  =  Final velocity

    u  = initial velocity

    Velocity – time Graph

    The area under the graph of a velocity – time graph is  displacement

    capture2

    Since the diagram is a trapezium, we can calculate the total distance using the area of a trapezium

    Let look at an example

    capture3

    From the diagram above

    i  what is the distance travelled during the first 10s

    ii the total distance travelled

    iii the average speed for the whole journey

    Solution

    i  using triange AOP = 1/2 * OP * AP = 1/2 * b * h = 1/2 * 10*30 = 150m

    ii using Trapezium AOCBA = 1/2 *(AB + OC) * AP = 1/2 *(20 + 42) *30 = 1/2 * 62 *30 = 930m

    ii average speed = total distance / total time taken

    total time taken is 42s

    average speed = 930 / 42 = 22.1 ms-1

    Derive, from the definitions of velocity and acceleration, equations that represent uniformly accelerated motion in a straight line

    v =u+at

    s=[(u+v)/2]t

    v2=u2+2as

    s=ut+1/2at2

     

    v = final velocity

    u = initial velocity

    t = time taken

    s = distance covered

    a = uniform acceleration

    From the definition of acceleration

    a = (v-u) / t

    Cross multiply and rearrange

    v = u + at

    From average velocity,

    Average velocity = s / t

    Average velocity = (v +u)/2

    equate the two equations together, you get

    s / t = (v +u)/2

    Cross multiply and rearrange

    s = [(v + u)t]/2

    Taking v = u + at ………i , and s = [(v + u)t]/2….ii

    Substiturte v = u + at in eqn i into eqn ii, so you get,

    s = ut + 1/2at2

    Taking v = u + at…….i and s = [(v – u)t]/2…. ii

    Make t the subject of the eqn in eqn i

    t = (v – u) / a …………iii

    substitute eqn iii into eqn ii, you get

    v2=u2+2as

    Motion of bodies falling in a uniform gravitational field without air resistance – Kinematics

    Motion of bodies falling in a uniform gravitational field without air resistance

    In a uniform gravitational field, the gravitational field strenght is constant. The gravitational field strenght is also refer to as acceleration due to gravity (g).

    Without air resistance means the air resistance is negligible or the drag force

    The displacement – time graph, velocity – time graph, acceleration – time graph of such a motion is shown below

    images

    Always remember that the gradient or slope of displacement – time graph is velocity, the gradient of velocity-time graph is acceleration.

    From the graph above, the acceleration-time graph shows that it is a uniform acceleration or a constant acceleration.

    v =u+at

    s=[(u+v)/2]t

    v2=u2+2as

    s=ut+1/2at2

    in this case all you have to do is make a = 9.81ms-2, which the value of acceleration due to gravity. But in some cases you can be ask to make a = 10ms-2

    The motion of bodies falling in a uniform gravitational field with air resistance

    The motion of bodies falling in a uniform gravitational field with air resistance
    image from xtremepapers.com

    When any object moves through air, the air offers a frictional resistance (drag) to the motion. This causes the object to decelerate. The deceleration is not constant but depends on the velocity of the object. The faster the object the greater the resistance and deceleration. You can experience this when you run – the faster you run, the harder the air seems to blow against.

    Graphical representaion of this kind on motion is shown below

    slideplayer.com/slide/2382797/
    image from slideplayer.com/slide/2382797/

    Where the arrow pointed shows the graph of displacement-time graph, velocity-time graph, acceleration-time graph when there is air resistance.

    For displacement-time graph: it takes more time to cover because of the air resistance compared with when there is no air resistance

    For velocity: the acceleration isnt constant because as the speed increases the air resistance increases until a time is reached when the the weight of the object equals the drag force(air resistance), at this point no resultant force acting on the body and it will fall with a constant speed, called the terminal velocity(this has being explained when i discussed dynamics)

    Terminal velocity is the point at which the resultant force is zero.

    Motion due to a uniform velocity in one direction and a uniform acceleration in a perpendicular direction.

    The type of motion to discuss here is a Projectile. Projectile is any object that is given an initial velocity and then follows a path determined entirely by gravitational acceleration.

    Motion due to a uniform velocity in one direction

    The initial velocity is at an angle of  θ. This initial velocity will be resolve into both vertical component and horizontal component.

    slide_19

    Using your SOHCAHTOA

    the vertical component of the velocity will be usinθ

    the horizontal component of the velocity will be ucosθ

    horizontal component of the velocity has no force acting so it is constant

    vertical component of the velocity has a constant force acting so there is a constant acceleration.

    derivations

    To calculate the time to reach the maximum height

    v = u – at

    at maximum height v = 0

    0 = usinθ – at

    t = usinθ / a

    your a = 9.81ms-2

    Time of flight = 2*t = 2usinθ / a

    To calculate maximum height

    v2=u2 – 2as

    at maximum height v = 0

    u = usinθ

    a = 9.81ms-2

    s = maximum height

    if you subsitute you get your maximum height

    Horizontal distance (range)

    v = d / t

    the reason for this formula is because there is no force acting on it, which implies a uniform velocity

    d= horizontal distance

    v = horizontal component of velocity = ucosθ

    t = time to complete the parabolic path ( which can be sometimes time of flight or time to reach the maximum height depending on the projectile diagram given). if it is a full diagram you use time of flight. if it is half of the full diagram you use time to reach the maximum height). The diagram above is a full diagram.

    ucosθ = d / t

    Recommended: Solved questions on motion

  • Simple Harmonic Motion Definition, Formulas, And Graphs

    Simple Harmonic Motion Definition, Formulas, And Graphs

    In this article, I will discuss the definition of simple harmonic motions, formulas, and graphs. Oscillation is one complete movement from the starting or rest position, up, then down and finally back up to the rest position. Examples are pendulum, the beating of the heart, vibration of a guitar string, the motion of a child on a swing e.t.c.

    A free oscillation means:

    • No energy loss
    • No external force acting
    • Constant energy
    • Constant amplitude

    Definition Of Simple Harmonic Motion

    It is defined as the motion of a particle about a fixed point such that its acceleration a is proportional to its displacement x from the fixed point, and is directed towards the point.
    Mathematically,

    capture1

    The negative sign tells us that the acceleration is always in opposite direction to the displacement x

    capture2

    The slope or gradient of this graph = ω^2

    Conditions necessary for a body to execute S.H.M

    • when the body is displaced from equilibrium, there must exist a restoring force
    • this restoring force must be proportional to the displacement of the body

    (it is always directed to the equilibrium position)

    a is acceleration

    x is the displacement

    Simple Harmonic Motion Formula

    The major formula in SHM is capture1

    the w = 2 pi f where w is angular frequency (unit rad/s) and f is the frequency (unit Hertz)

    Also, in S.H.M we can have v = wx, where v is the velocity and x is the displacement.

    capture

    capture

    capture

    Understanding of terms
    Period : it is the time taken for one complete oscillation
    Frequency: it is the number of oscillations per unit time
    Amplitude : it is the maximum displacement from the rest position.
    Displacement : it is the distance from the equilibrium position
    F= 1/T unit is Hertz (Hz)
    F is frequency, T is period

    capture

    Displacement And Velocity in Simple Harmonic Motion

    Displacement and velocity in S.H.M varies with each other. The velocity is always maximum at the equilibrium position. Also, the displacement is maximum when the velocity is zero.

    Simple Harmonic Motion Graphs

    capture

    This means when displacement is maximum, velocity is zero and acceleration maximum but in opposite direction.

    capture

    capture

    V is the instantaneous speed
    Interchange between Kinetic and potential energy
    K. E is maximum when displacemet is zero
    P.E is maximum when the displacement is maximum

    capture

    capture

    Damping

    Damping is an influence within or upon an oscillatory system that has the effect of reducing oscillations

    It can now be properly define as reduction in energy of oscillations/ reduction in amplitude due to force opposing motion/ resistive force.

    Note

    During damping amplitude of oscillation does not decrease linearly also the frequency of the oscillations does not change as the amplitude decreases.

    Types of Damping

    Light damping: Amplitude decreases gradually as the oscillations continues for a long time

    img_full_46609

    Critical damping: displacement decreases to zero in the shortest time without oscillation

    Over damping : displacement decreases to zero in a longer time than for critical damping without any oscillation

    capture

    Forced oscillation

    This occur when an external force is applied to the original frequency causing a change in the frequency of the oscillation

    For resonance to occur, there must be a system capable of oscillating freely and also have a way in which the system is forced to oscillate.

    some terms

    forced frequency: frequency at which object is made to vibrate

    natural frequency of vibration: frequency at which object vibrates when free to do so

    Resonance

    resonance occurs when the natural frequency of vibration of an object is equal to the driving frequency giving a maximum amplitude of vibration

    capture

    Uses of resonance

    oscillation of a child’s swing

    microwave to cook food

    tuning of radio receiver

    Problems of resonance

    high-pitched sound waves can shatter fragile object

    metal panels on machinery vibrate

  • How to solve questions on Kinematics and deformation of solids

    How to solve questions on Kinematics and deformation of solids

    How to solve questions on Kinematics and deformation of solids

    Question 1

    A train with an initial velocity of 20ms-1 is subjected to a uniform deceleration of 2ms-2. The time required to bring the train to a complete halt is
    A. 40s         B. 5s            C. 10s          D. 20s

    Solution

    initial velocity = 20 ms-1

    final velocity = 0 ms-1 ( since the train completely come to a halt)

    deceleration = 2ms-1

    V = u + at

    0 = 20 + (-2) * t

    -20 = -2t

    t = 20/2  = 10 s

    C is the correct option

    Question 2

    Calculate the work done, when a force of 20N stretches a spring by 50mm.
    A. 2.5 J      B. 0.5 J         C. 1.5 J        D. 2.0 J

    Solution

    workdone = 1/2 f e

    f = 20 N

    e = 50 mm = 0.05 m

    workdone = 1/2 * 20 * 0.05   =  0.5 J

    B is the correct option

    Question 3 and 4 are from UTME 2012 Physics Questions – Type Yellow

    Question 3

    A car starts from rest and moves with a uniform acceleration of 30ms-2 for 20s. Calculate the distance covered at
    the end of the motion.
    A. 6km        B. 12km         C. 18km            D. 24km.

    Solution

    initial velocity = 0 ms-1 ( since it is starting from rest)

    acceleration = 30 ms-1

    time taken = 20 s

    using

    s = ut + 1/2at^2

    s =0 + 1/2 * 30 * 20^2

    s = 400*15

    s = 6000 m  = 6 km

    A is the correct option

    Question 4

    If a load of 1kg stretches a cord by 1.2cm, what is the force constant of
    the cord?
    A. 866 Nm-1          B. 833 Nm-1           C. 769 Nm-1             D. 667 Nm-1

    Solution

    Mass = 1kg

    weight = mg = 1 * 10 = 10 N

    extension = 1.2 cm  = 0.012 m

    force constant = f / e

    k = 10 / 0.012

    k = 833 Nm-1

    B is the correct option

    Question 5

    This question is from advance physics Nelkon and parker

    A car moving with a velocity of 36 kmh-1 accelerates uniformly at 1 ms-2 until it reaches a velocity of 54 kmh-1. Calculate

    i the time taken

    ii the distance travelled during the acceleration

    Solution

    x kmh-1 to ms-1 = (x *1000) / 3600

    36 kmh-1 = (36 * 1000) / 3600 = 10 ms-1

    54 kmh-1 = (54 * 1000) / 3600 = 15 ms-1

    initial velocity = 10 ms-1

    final velocity = 15 ms-1

    v = u + at

    15 = 10 + 1t

    t = 15 – 10

    t = 5 s

    ii

    v^2 = u^2 + 2as

    15^2 = 10^2 + 2*1*s

    225 = 100 + 2s

    2s = 225 – 100

    2s = 125

    s = 62.5 m

    Recommended: Short note on Kinematics

  • How to solve questions on oscillation for Cambridge A level

    How to solve questions on oscillation for Cambridge A level

    cambridge oct/nov 2006 p4

    Q1

    Two vertical springs, each having spring constant k, support a mass. The lower spring is
    attached to an oscillator as shown below

    capture

    The oscillator is switched off. The mass is displaced vertically and then released so that it
    vibrates. During these vibrations, the springs are always extended. The vertical acceleration
    a of the mass m is given by the expression
    ma = –2kx,
    where x is the vertical displacement of the mass from its equilibrium position.
    Show that, for a mass of 240 g and springs with spring constant 3.0Ncm–1, the
    frequency of vibration of the mass is approximately 8Hz

    Solution

    mass = 240g = 0.24kg

    k = 3.0 Ncm-1 = 300 Nm-1

    ma = –2kx

    capture1……….i

    0.24*a = -2* 300* x

    a = -600x / 0.24

    a = 2500x

    substitute for a in equ i

    capture

    find the square root of both sides

    capture

    f = 8 Hz

    The question is from cambridge may/june 2014 p41

    A student investigates the energy changes of a mass oscillating on a vertical spring, as shown below

    capture

    The student draws a graph of the variation with displacement x of energy E of the oscillation, as shown below

    capture

    The student repeats the investigation but with a smaller amplitude. The maximum value of E
    is now found to be 1.8 mJ.
    Use graph above to determine the change in the amplitude

    Solution

    From the graph the maximum kinetic energy = 2.4 mJ

    Change in Kinetic energy = 2.4 – 1.8 = 0.6 mJ

    capture

    capture

    Amplitude = 1.5 cm = 0.015 m

    capture

    When the amplitude change maximum energy E is 1.8m J

    capture

    Change in Amplitude = 1.5 cm – 1.3 cm

    change in amplitude = 0.2 cm