Physics Notes on Work, Energy and Power

Ch 6. Work and Energy

  • Learning Outcomes:
    • Work
    • Kinetic energy
    • Work-Energy Principle
    • Potential energy
    • Conservation of energy
    • Power
    • Problem solving

Work

  • Definition of work in physics differs from everyday language.
  • Work is accomplished when a force moves an object through a certain distance.

Work Done by a Constant Force

  • W=FdcosθW = Fd \cos\theta
  • W=FdW = \vec{F} \cdot \vec{d}
    • Where FcosθF \cos\theta is the component of the force parallel to the displacement dd.
  • SI Unit of work is joule (J)
    • 1J=1N.m1 J = 1 N.m

Example

  • Movers pushing a 160 kg crate 10.3 m across a rough floor without acceleration, with μk=0.50\mu_k = 0.50
  • Free body diagram shows forces acting on the crate.
  • Net force in the x-direction: F<em>x=Ff</em>k=ma=0\sum F<em>x = F - f</em>k = ma = 0
  • Therefore, F=fkF = f_k
  • Friction force: f<em>k=μ</em>kN=μkmgf<em>k = \mu</em>k N = \mu_k mg
  • Work done: W=Fdcosθ=μkmgdcos(0)W = Fd \cos\theta = \mu_k mgd \cos(0^{\circ})
  • W=0.50×160×9.8×10.3×cos(0)=8.1×103JW = 0.50 \times 160 \times 9.8 \times 10.3 \times \cos(0^{\circ}) = 8.1 \times 10^3 J

Exercise

  • Minimum work needed to push a 950 kg car 810 m up a 9.0° incline.
    • (a) ignore friction
    • (b) include friction, μk=0.25\mu_k = 0.25
  • Free body diagram shows forces acting on the car on an incline.
  • Net force in the x-direction: Fx=Fmgsinθ=0\sum F_x = F - mg \sin\theta = 0
  • Net force in the y-direction: Fy=Nmgcosθ=0\sum F_y = N - mg \cos\theta = 0
  • Minimum work occurs when the car is moved with constant velocity.
  • (a) When friction is ignored:
    • W=Fd=mgsinθ×dW = Fd = mg \sin\theta \times d
    • W=950×9.8×sin(9.0)×810m=1.2×106JW = 950 \times 9.8 \times \sin(9.0^{\circ}) \times 810 m = 1.2 \times 10^6 J
  • (b) When friction is included:
    • F<em>x=Fmgsinθf</em>k=0\sum F<em>x = F - mg \sin\theta - f</em>k = 0
    • F=mgsinθ+fkF = mg \sin\theta + f_k
    • f<em>k=μ</em>kN=μkmgcosθf<em>k = \mu</em>k N = \mu_k mg \cos\theta
    • F=mgsinθ+μkmgcosθF = mg \sin\theta + \mu_k mg \cos\theta
    • W=Fd=(mgsinθ+μkmgcosθ)dW = Fd = (mg \sin\theta + \mu_k mg \cos\theta)d
    • W=(950×9.8×sin(9.0)+0.25×cos(9.0))×810m=3.0×106JW = (950 \times 9.8 \times \sin(9.0^{\circ}) + 0.25 \times \cos(9.0^{\circ})) \times 810 m = 3.0 \times 10^6 J
  • Note: Work in part (b) is more than part (a), as expected, because some of the work is done to overcome friction.

Energy

  • Energy: The ability to do work.
  • Kinetic Energy (KE):
    • The energy of an object by virtue of its motion.
    • KE=12mv2KE = \frac{1}{2} mv^2 (translational KE only)
  • Potential Energy (PE):
    • The energy of an object by virtue of its position or configuration.
    • Gravitational Potential Energy (GPE): mghmgh
    • Elastic Potential Energy: 12kx2\frac{1}{2} kx^2
  • Translational motion: objects moving without rotation

Work - Energy Principle

  • Net work done on an object is equal to the change in its KE.
  • W<em>net=K</em>fKi=ΔKW<em>{net} = K</em>f - K_i = \Delta K
  • W<em>net=F</em>netdW<em>{net} = F</em>{net} d
  • K<em>i=12mv</em>i2K<em>i = \frac{1}{2} mv</em>i^2
  • K<em>f=12mv</em>f2K<em>f = \frac{1}{2} mv</em>f^2
  • W<em>net=12mv</em>f212mvi2W<em>{net} = \frac{1}{2} mv</em>f^2 - \frac{1}{2} mv_i^2
  • A net force accelerates an object from v<em>iv<em>i to v</em>fv</em>f over a displacement dd.

Exercise

  • A 1500 kg car traveling at 17 m/s can brake to a stop within a distance of 20 m.
  • How much work is done by the friction force?
    • W=ΔK=K<em>fK</em>iW = \Delta K = K<em>f - K</em>i
    • W=12mv<em>f212mv</em>i2W = \frac{1}{2} mv<em>f^2 - \frac{1}{2} mv</em>i^2
    • W=012×1500×(17)2=2.2×105JW = 0 - \frac{1}{2} \times 1500 \times (17)^2 = -2.2 \times 10^5 J
  • The direction of the friction force: opposite to the direction of motion.

Exercise

  • A person accelerates a 50 kg box from 0.5 m/s to 2.5 m/s over a distance of 2.0 m.
    • (a) How much work is done by the person?
    • (b) How much force is applied by the person? Assume no friction.
  • (a) Work done by the person:
    • W=ΔK=K<em>fK</em>iW = \Delta K = K<em>f - K</em>i
    • K<em>i=12mv</em>i2K<em>i = \frac{1}{2} mv</em>i^2
    • K<em>f=12mv</em>f2K<em>f = \frac{1}{2} mv</em>f^2
    • W=12×50×(2.5)212×50×(0.5)2W = \frac{1}{2} \times 50 \times (2.5)^2 - \frac{1}{2} \times 50 \times (0.5)^2
    • W=1.5×102JW = 1.5 \times 10^2 J
  • (b) Force applied by the person:
    • W=FdcosθW = Fd \cos\theta
    • F=Wdcosθ=1.5×1022.0×cos(0)=75.1NF = \frac{W}{d \cos\theta} = \frac{1.5 \times 10^2}{2.0 \times \cos(0^{\circ})} = 75.1 N

Potential Energy

  • ΔPE=mgh\Delta PE = mgh (relative to ground)
  • Work done by the person in lifting the brick: W=Fdcosθ=mg(y<em>fy</em>i)W = Fd \cos\theta = mg(y<em>f - y</em>i)
  • y<em>fy</em>i=hy<em>f - y</em>i = h
  • The value of GPE depends on where we specify the ground level.
  • The work done in lifting the brick is equal to the change in GPE.

Conservation of Mechanical Energy

  • Total mechanical energy E of a system remains constant.
  • E=K+P=constantE = K + P = constant
  • K<em>i+P</em>i=K<em>f+P</em>fK<em>i + P</em>i = K<em>f + P</em>f

Example

  • A 2.0 kg block is dropped from h = 3.0 m.

    • What is its KE and PE at
      • a) Height 1.0 m
        • PE=mgh=2×9.8×1=19.6JPE = mgh = 2 \times 9.8 \times 1 = 19.6 J
      • b) Ground level

    *Consider a block being dropped from a height of 3 meters.

    • At a height of 3 meters, the potential energy (PE) is:
      • PE=mgh=2×9.8×3=58.8JPE = mgh = 2 \times 9.8 \times 3 = 58.8 J

    *Based on the principle of conservation of mechanical energy:
    * K+P=constantK + P = constant

    *Therefore, at a height of 1 meter:
    * PE=mgh=2×9.8×1=19.6JPE = mgh = 2 \times 9.8 \times 1 = 19.6 J
    * KE = Total Energy - PE at 1m
    * KE = 39.2 J at 1m

Exercise

  • A pendulum with m = 0.2 kg is released from height 0.5 m from its equilibrium position.
    • What is the speed of the bob at the equilibrium position?
      • E=K+P=constantE = K + P = constant
      • EA=K+PE_A = K + P
      • EB=K+PE_B = K + P
      • v=2gh=2×9.8×0.5=3.1m/sv = \sqrt{2gh} = \sqrt{2 \times 9.8 \times 0.5} = 3.1 m/s

Example

  • A child of mass 24 kg slides on a 6.0 m high slide starting from rest.
    • What is the speed of the child at the bottom of the slide?
      • Assume slide is frictionless.
        • KE<em>f+PE</em>f=KE<em>i+PE</em>iKE<em>f + PE</em>f = KE<em>i + PE</em>i
        • PE=0PE = 0
        • v=mgh=2×9.8×6=10.8m/sv = \sqrt{mgh} = \sqrt{2 \times 9.8 \times 6} = 10.8 m/s

Quiz

  • What will be the final speed if another child with twice the mass slides down?
    • Final speed of both children will be the same, as mass cancels out in the CME equation.
  • Will the final speed be greater or smaller if friction is present?
    • Smaller, as some of the energy is used up in overcoming friction.

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Power

  • The time rate of doing work is called power.
    • P=WtP = \frac{W}{t}
    • The average power due to the force is:
      • P=FdtP = \frac{F \cdot d}{t}
      • P=FvP = F \cdot v

Example

  • How long will it take a 1750 W motor to lift a 285 kg piano to a sixth-story window 16.0 m above?
    • P=Wt=mghtP = \frac{W}{t} = \frac{mgh}{t}
    • t=mghP=285×9.8×16.01750=25.5st = \frac{mgh}{P} = \frac{285 \times 9.8 \times 16.0}{1750} = 25.5 s

Exercise

  • A shot putter accelerates a 7.3 kg shot from rest to 14 m/s. If this motion takes 1.5 s, what average power was developed?
    • P=ΔKt=12mv<em>f212mv</em>i2tP = \frac{\Delta K}{t} = \frac{\frac{1}{2} mv<em>f^2 - \frac{1}{2} mv</em>i^2}{t}
    • P=12×7.3×(14)21.5=4.8×102WP = \frac{\frac{1}{2} \times 7.3 \times (14)^2}{1.5} = 4.8 \times 10^2 W