DE4101 Work Power Energy

download DE4101 Work Power Energy

of 18

Transcript of DE4101 Work Power Energy

  • 7/25/2019 DE4101 Work Power Energy

    1/18

    Jonathan Leaver PhD

  • 7/25/2019 DE4101 Work Power Energy

    2/18

    TheoryWork When a force F moves an object of mass m through a distance s work is performed.

    The amount of work is determined from the formula

    Work (Joules) = Force (N) x distance (m) or W = F x s

    1 Joule = 1 N-m

    Power Power (Watts) = work (J)/time (s) 1

    or P = W/t

    = Fx

    s/tP = F x v

    Power = force x velocity 2

  • 7/25/2019 DE4101 Work Power Energy

    3/18

    Theory (cont.)Energy A law of physics developed in the modern day by Albert Einstein

    states that energy can neither be created nor destroyed it can onlybe transformed from one form to another.

    Energy can take many forms:

    Chemical, potential, kinetic, nuclear, heat, mechanical, electrical,

    electromagnetic

    Potential energy is energy possessed by an object due to its position

    relative to a fixed datum or height.

    Kinetic energy is energy possessed by an object due to its motion

  • 7/25/2019 DE4101 Work Power Energy

    4/18

    Theory (cont.)Energy is transformed from one form to

    another in hydro projects

    The water behind the dam has

    potential energy.

    When the water travels into the

    penstocks some of the potential

    energy is converted into kinetic energy

    When the water turns the turbine

    blade some of the kinetic energy of

    the water is converted to kineticenergy in the turbine.

    Some of the turbine energy is lost by

    heat emission from friction in the shaft

    bearings.

    Much of the rest of the

    turbine energy is converted to

    electrical energy.

  • 7/25/2019 DE4101 Work Power Energy

    5/18

    Theory (cont.)Calculate Energy of Motion (Kinetic Energy)

    Now F = m a ...... 3

    Also = + 2

    Hence a =

    Consider an object initially at rest. Then u = 0 and a =

    Substituting for a in equation 3 above gives:

    F = m

    But W = F x s

    Therefore W = KE (Kinetic Energy) =1

    mv2 .4

  • 7/25/2019 DE4101 Work Power Energy

    6/18

    Theory (cont.)Calculate Potential Energy due to gravity

    Now F = m a .. 3

    Acceleration = gravity = g (9.81 m/s2)

    Therefore F = mg

    But W = F x s

    where s is the height above ground level i.e. s = h.

    Therefore W = PE (Potential Energy) = mgh 5

  • 7/25/2019 DE4101 Work Power Energy

    7/18

    SpringsF = -kX where k = spring constant

    Energy = 0 = 1 kX2

    Source: http://www.thetrc.org/pda_content/texasphysics/e-BookData/Images/SB/58/LR/Spring%20Potential%20Energy.png

  • 7/25/2019 DE4101 Work Power Energy

    8/18

    Example 1: EnergyA steel ball bearing of mass 50 grams is dropped from a height of 2 metres on

    to a smooth, flat, rigid plate and rebounds to a height of 1.75 metres.

    Calculate (i) Its original potential energy (ii) Its kinetic energy the instant

    before it hits; (iii) Its kinetic energy the instant it starts to rebound; (iv) Itsvelocity on impact. How do you account for energy lost in the collision of ball

    and ground?

    1.75m 2m

    mass=50 g

    Solution

    (i) The original potential energy of the ball, using the

    plate as a datum isPE = mgh = 0.05 x 9.81 x 2 = 0.981 Joules (J)

    (ii) KE at the instant it hits is the same as the PE at the

    start as no energy has been lost only transformed.

    KE = 0.981 J

  • 7/25/2019 DE4101 Work Power Energy

    9/18

    Example 1: Energy (cont.)

    1.75m 2m

    mass=50 g

    (iii) After impact the KE will equal the PE at the

    maximum height it rises to.

    PE = mgh = 0.05 x 9.81 x 1.75 = 0.858 J

    (iv) The velocity on impact is determined from kinetic

    energy.

    KE = 0.5mv2 = 0.981 JTherefore v2 = (0.981 x 2)/0.05 = 39.24

    and v = 6.26 m/s

    (v) Energy is lost at the point of impact in heat and

    noise by deformation of the ball.

  • 7/25/2019 DE4101 Work Power Energy

    10/18

    Example 2: Work = 600

    F = 400 N

    Work is only done in the direction of

    movement by the component of force in

    that direction.

    Consider an object moving 20 m under a

    force of 400 kN acting at an angle of 60

    degrees to the horizontal.

    WD = force x distance = FcosF x s= 0.4(kN)cos60 x 20m

    = 4.00 kJ

  • 7/25/2019 DE4101 Work Power Energy

    11/18

    Example 3: Power

    An electrically driven conveyor belt carries a 60,000 packages per hour adistance of 80 m up an incline of 1 in 12. Each package weighs 48 N and the

    power absorbed by friction in the drive is 2 kW. What is the power output of the

    motor?

    sin = 1/12

  • 7/25/2019 DE4101 Work Power Energy

    12/18

    Example 3: Power (cont.)An electrically driven conveyor belt carries a 60,000 packages perhour a distance of 80 m up an incline of 1 in 12. Each package weighs

    48 N and the power absorbed by friction in the drive is 2 kW. What is

    the power output of the motor?

    sin = 1/12(i) To determine the power output of the

    motor determine firstly how much work is

    done on each package and then how long it

    takes to do this work.

    (ii) Then we can use the formula

    Power = Work/time

    (iii) Work = force x distance where the force

    must act in the direction of movement.

    The force in this case is gravity.

    The component of weight of one

    package in the direction of the

    conveyor = mgsin

    mg

    mgsin

  • 7/25/2019 DE4101 Work Power Energy

    13/18

    Example 3: Power (cont.)An electrically driven conveyor belt carries a 60,000packages per hour a distance of 80 m up an incline of 1 in

    12. Each package weighs 48 N and the power absorbed

    by friction in the drive is 2 kW. What is the power output

    of the motor?

    sin = 1/12

    The time each package takes on the belt is

    t = 3600/60,000 = 0.06 s

    The power ignoring friction

    P = WD/t = Fsin *s/t

    = 48(1/12) x 80/0.06= 5.333 kW

    However we are given 2 kW is lost in friction

    therefore total power required is:

    P = 5.333 + 2

    = 7.333 kW

  • 7/25/2019 DE4101 Work Power Energy

    14/18

    Example 4: Power (Dodd & Richardson Ch7 No. 6 pg 99)

    A diesel-electric locomotive of mass 300 tonnes and tractive resistance 120 N/ttravels up a 1:100 slope at 60 km/h. The train pulls carriages with a mass of 700

    tonnes and tractive resistance 50 N/t. Find the power developed at the driving

    wheels. Ans. 2.818 MW

    120N/t

    300 t

    50 N/t

    700 t

    Slope1 in 100

  • 7/25/2019 DE4101 Work Power Energy

    15/18

    Solution: Power (Dodd & Richardson Ch7 No. 6 pg 99)

    mg

    mgsin

    Power = force (up slope) * velocity (up slope)

    We must find the force exerted by the wheels to

    overcome gravity and tractive resistance.

    Summing forces up the slope

    Fengine(300+700)gsin (120*300+700*50)/1000 = 0

    Fengine = 169.1 kN

    Power = F * v = 169.1 kN * 60/3.6 m/s = 2.818 MW

    120N/t

    300 t

    50 N/t

    700 t

    Slope1 in 100

    Fengine

  • 7/25/2019 DE4101 Work Power Energy

    16/18

    Problem 5 (Ivanoff 20.1)A 180 tonne train climbs an incline of 1.5o for 2 km. Its

    initial velocity before the climb is 90 km/h. The tractive

    effort exerted by the engine is 53.2 kN and tractive

    resistance is 95 N/t. Determine the final speed after the

    climb.Ans: 72 km/h

  • 7/25/2019 DE4101 Work Power Energy

    17/18

    Problem 6: (Ivanoff 20.13)A stationary 18 kg block sides down a 30 degree slope a

    distance of 2.5 m where it compresses a spring with

    stiffness 2.7 N/mm also aligned at 30 degrees. If the

    coefficient of friction between the block and the surface is

    0.2 find how much the spring will be compressed.

    Ans: 349 mm Hint: Use energy and work done

  • 7/25/2019 DE4101 Work Power Energy

    18/18

    Self StudyCh 7 (Dodd and Richardson)

    (p 99&100) 3,4,5,9,10,15,16,17