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Chapter 6: Work and Energy

6.1: Work Done by a Constant Force

  • Work is a force applied over a distance.

    • Work = force x displacement

      • W=FsW=Fs

    • Scalar quantity

    • SI Unit: joule (J)

      • 1Nm=1joule(J)1N\cdot m=1joule\left( J\right)

  • Definition of work:

    • W=FcosθsW=F\cos \theta s

      • FF = force of the object

      • ss = displacement

      • θ\theta = angle between F\overrightarrow{F} and s\overrightarrow{s} when places tail to tail.

      • cos0\cos0 = 1

      • cos90\cos90 = 0

      • cos180\cos180 = -1

  • When a force is PARALLEL to the displacement, the work by the force is POSITIVE.

  • When a force is OPPOSITE to the displacement, the work done by the force is NEGATIVE.

  • When the force is PERPENDICULAR to the displacement, the work done by the force is ZERO.


6.2 The Work Energy Theorem and KE

  • The kinetic energy (KE) of an object with mass m and speed v is given by:

    • KE=12mv2KE=\dfrac{1}{2}mv^{2}

    • KE will always be positive because mass can not be negative and v² is always positive.

    • Scalar quantity

    • SI Unit: J

  • The work-energy theorem - the net work done by the forces on an object equals the change in its kinetic energy.

    • When a net external force does work on an object, the kinetic energy of the object changes by the amount of work done on it:

      • W=KEfKE0W=KE_{f}-KE_{0}


6.3: Gravitational Potential Energy

  • Gravitational potential energy - the energy that an object of mass m has by virtue of its position relative to the surface of the earth.

    • Wgravity=mgh0mghfW_{gravity}=mgh_{0}-mgh_{f}

  • That position is measured by the height hh of the object relative to an arbitrary zero level:

    • PE=mghPE=mgh

    • Scalar quantity

    • SI Unit: J

  • Potential and Kinetic energy

    • When your PE is at maximum, your KE is zero.

    • When your PE is zero, your KE is at maximum.


6.4: Conservative vs. Nonconservative Forces

Conservative Forces

  • The gravitational force is called a conservative force and occurs when:

    • The work it does on a moving object is independent of the path between the object’s initial and final positions.

    • It does no work on an object moving around a closed path, starting and finishing at the same point.

  • The total mechanical energy (kinetic energy + potential energy) of the system remains constant if only conservative forces are acting on it.

  • Gravity is a conservative force. It does no work on an object, executing a closed path.

  • When a path has the same starting and ending point, it is called a closed path.

    • For a closed path, the work done by gravity will equal zero joules.

    • Wgravity = 0 J for a closed path.

Working Together

  • When conservative forces and nonconservative forces act simultaneously on an object, we can write work as:

    • W=Wc+WncW=W_{c}+W_{nc}

Conservative vs Nonconservative Table

Conservative

Nonconservative

Work done is independent of path.

Work done is path dependent.

Mechanical energy is conserved.

Mechanical energy is not conserved

The work done in a closed loop is zero.

The work done in a closed loop may not be zero.

PE can be defined.

PE can not be defined.

The force is independent of the velocity of an object.

The force depends on the positions and velocities of the objects.

Examples: gravity, spring

Examples: friction, tension, air resistance, normal force


6.5: The Conservation of Mechanical Energy

  • If the net work on an object by nonconservative forces is zero, then its energy does not change.

  • Conservation of energy: Ef=E0E_{f}=E_{0}

    • This equation can also broken down into: 12mvf2+mghf=12mv02+mgh0\dfrac{1}{2}mv_{f}^{2}+mgh_{f}=\dfrac{1}{2}mv_{0}^{2}+mgh_{0}

  • Total mechanical energy: E=KE+PEE=KE+PE

    • The total mechanical energy of an object remains constant as the object moves, provided that the net work done by external nonconservative forces is zero


6.6: Nonconservative Forces and the Work-Energy Theorem

  • Most moving objects experience nonconservative forces, such as friction, air resistance, and propulsive forces, and the work Wnc done by the net external nonconservative force is not zero. In these situations, the difference between the final and initial total mechanical energies is equal Wnc. Can be written in two ways:

    • Wnc=EfE0W_{nc}=E_{f}-E_{0}

    • Wnc=(mghf+12mvf2)(mgh0+12mv02)W_{nc}=\left( mgh_{f}+\dfrac{1}{2}mv_{f}^{2}\right) -\left( mgh_{0}+\dfrac{1}{2}mv_{0}^{2}\right)

  • The concept of potential energy is not defined for a nonconservative force.


6.7: Power

  • Average power (P\overline{P}) is the time rate at which work is done.

    • It is defined as Work divided by time.

    • P=Wt\overline{P}=\dfrac{W}{t}

      • W is also equal Fs

      • s/t is equal to v\overline{v}

      • Another way to write this equation is P=Fv\overline{P}=F\overline{v}

    • Scalar quantity

    • SI Unit: watt (W) aka joule/s

  • The work–energy theorem relates the work done by a net external force to the change in the energy of the object.

    • We can also define average power as the rate at which the energy is changing, or as the change in energy/time during which the change occurs.

  • 1 horsepower = 550ftlbs/sec550ft\cdot lbs/\sec = 745.7 watts


6.8: Other Forms of Energy and the Conservation of Energy

The Principle of Conservation of Energy

  • Energy can neither be created nor destroyed, but can only be converted from one form to another.

S

Chapter 6: Work and Energy

6.1: Work Done by a Constant Force

  • Work is a force applied over a distance.

    • Work = force x displacement

      • W=FsW=Fs

    • Scalar quantity

    • SI Unit: joule (J)

      • 1Nm=1joule(J)1N\cdot m=1joule\left( J\right)

  • Definition of work:

    • W=FcosθsW=F\cos \theta s

      • FF = force of the object

      • ss = displacement

      • θ\theta = angle between F\overrightarrow{F} and s\overrightarrow{s} when places tail to tail.

      • cos0\cos0 = 1

      • cos90\cos90 = 0

      • cos180\cos180 = -1

  • When a force is PARALLEL to the displacement, the work by the force is POSITIVE.

  • When a force is OPPOSITE to the displacement, the work done by the force is NEGATIVE.

  • When the force is PERPENDICULAR to the displacement, the work done by the force is ZERO.


6.2 The Work Energy Theorem and KE

  • The kinetic energy (KE) of an object with mass m and speed v is given by:

    • KE=12mv2KE=\dfrac{1}{2}mv^{2}

    • KE will always be positive because mass can not be negative and v² is always positive.

    • Scalar quantity

    • SI Unit: J

  • The work-energy theorem - the net work done by the forces on an object equals the change in its kinetic energy.

    • When a net external force does work on an object, the kinetic energy of the object changes by the amount of work done on it:

      • W=KEfKE0W=KE_{f}-KE_{0}


6.3: Gravitational Potential Energy

  • Gravitational potential energy - the energy that an object of mass m has by virtue of its position relative to the surface of the earth.

    • Wgravity=mgh0mghfW_{gravity}=mgh_{0}-mgh_{f}

  • That position is measured by the height hh of the object relative to an arbitrary zero level:

    • PE=mghPE=mgh

    • Scalar quantity

    • SI Unit: J

  • Potential and Kinetic energy

    • When your PE is at maximum, your KE is zero.

    • When your PE is zero, your KE is at maximum.


6.4: Conservative vs. Nonconservative Forces

Conservative Forces

  • The gravitational force is called a conservative force and occurs when:

    • The work it does on a moving object is independent of the path between the object’s initial and final positions.

    • It does no work on an object moving around a closed path, starting and finishing at the same point.

  • The total mechanical energy (kinetic energy + potential energy) of the system remains constant if only conservative forces are acting on it.

  • Gravity is a conservative force. It does no work on an object, executing a closed path.

  • When a path has the same starting and ending point, it is called a closed path.

    • For a closed path, the work done by gravity will equal zero joules.

    • Wgravity = 0 J for a closed path.

Working Together

  • When conservative forces and nonconservative forces act simultaneously on an object, we can write work as:

    • W=Wc+WncW=W_{c}+W_{nc}

Conservative vs Nonconservative Table

Conservative

Nonconservative

Work done is independent of path.

Work done is path dependent.

Mechanical energy is conserved.

Mechanical energy is not conserved

The work done in a closed loop is zero.

The work done in a closed loop may not be zero.

PE can be defined.

PE can not be defined.

The force is independent of the velocity of an object.

The force depends on the positions and velocities of the objects.

Examples: gravity, spring

Examples: friction, tension, air resistance, normal force


6.5: The Conservation of Mechanical Energy

  • If the net work on an object by nonconservative forces is zero, then its energy does not change.

  • Conservation of energy: Ef=E0E_{f}=E_{0}

    • This equation can also broken down into: 12mvf2+mghf=12mv02+mgh0\dfrac{1}{2}mv_{f}^{2}+mgh_{f}=\dfrac{1}{2}mv_{0}^{2}+mgh_{0}

  • Total mechanical energy: E=KE+PEE=KE+PE

    • The total mechanical energy of an object remains constant as the object moves, provided that the net work done by external nonconservative forces is zero


6.6: Nonconservative Forces and the Work-Energy Theorem

  • Most moving objects experience nonconservative forces, such as friction, air resistance, and propulsive forces, and the work Wnc done by the net external nonconservative force is not zero. In these situations, the difference between the final and initial total mechanical energies is equal Wnc. Can be written in two ways:

    • Wnc=EfE0W_{nc}=E_{f}-E_{0}

    • Wnc=(mghf+12mvf2)(mgh0+12mv02)W_{nc}=\left( mgh_{f}+\dfrac{1}{2}mv_{f}^{2}\right) -\left( mgh_{0}+\dfrac{1}{2}mv_{0}^{2}\right)

  • The concept of potential energy is not defined for a nonconservative force.


6.7: Power

  • Average power (P\overline{P}) is the time rate at which work is done.

    • It is defined as Work divided by time.

    • P=Wt\overline{P}=\dfrac{W}{t}

      • W is also equal Fs

      • s/t is equal to v\overline{v}

      • Another way to write this equation is P=Fv\overline{P}=F\overline{v}

    • Scalar quantity

    • SI Unit: watt (W) aka joule/s

  • The work–energy theorem relates the work done by a net external force to the change in the energy of the object.

    • We can also define average power as the rate at which the energy is changing, or as the change in energy/time during which the change occurs.

  • 1 horsepower = 550ftlbs/sec550ft\cdot lbs/\sec = 745.7 watts


6.8: Other Forms of Energy and the Conservation of Energy

The Principle of Conservation of Energy

  • Energy can neither be created nor destroyed, but can only be converted from one form to another.