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Rotational Equilibrium and Dynamics Chapter 8

Rotational Equilibrium and Dynamics

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Rotational Equilibrium and Dynamics. Chapter 8. Magnitude of a Torque. What is a torque? A quantity that measures the ability of a force to rotate an object around some axis. . r. Example…. Imagine opening a door around a hinge. The door is free to rotate about a fixed axis. - PowerPoint PPT Presentation

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Page 1: Rotational Equilibrium  and Dynamics

Rotational Equilibrium and Dynamics

Chapter 8

Page 2: Rotational Equilibrium  and Dynamics

Magnitude of a Torque

• What is a torque?– A quantity that measures the ability of a force to

rotate an object around some axis.

r

Page 3: Rotational Equilibrium  and Dynamics

Example…• Imagine opening a door around a hinge.• The door is free to rotate about a fixed axis.• This axis is the door’s axis of rotation• When an individual pulls the door open at the

handle with a force that is perpendicular to the door, the door opens.– The measurement of this force is the Torque of the

motion.

Page 4: Rotational Equilibrium  and Dynamics

Torque depends on a forceand a lever arm

• If someone opens the door from the previous example, but at a point closer to the hinge, the door would be much more difficult to rotate.

• How easily an object rotates depends on how much force is applied as well as WHERE the force is applied.

Page 5: Rotational Equilibrium  and Dynamics

Torque depends on a forceand a lever arm

• The farther the force is from the axis of rotation, the easier it is to rotate the object and the more torque is produced.

• The PERPENDICULAR distance from the axis of rotation to a line drawn along the direction of the force is called the lever arm, or moment arm.

Page 6: Rotational Equilibrium  and Dynamics

Torque and Lever Arm

d

F

axis of rotation

Angular speed

Force applied to an extended object can produce a torque.This torque in turn, causes this object to rotate.

Page 7: Rotational Equilibrium  and Dynamics

TORQUE Equation

• Torque also depends of the angle between a force and a lever arm

Torque = Force (lever arm)(sin theta)

T = Fd(sin 0)

**SI unit of torque: Newton meter or (N x m)

Page 8: Rotational Equilibrium  and Dynamics

Calculating Torque at an angle

F

d

F(sin )

T = d x (sin )

Page 9: Rotational Equilibrium  and Dynamics

Conceptual Question…

• 1: A student pushes with minimal force of 50.0 N on the middle of a door to open it.

– What minimum force must be applied at the edge of the door in order for the door to open?

– What minimum force must be applied to the dinged side of the door in order for the door to open?

Page 10: Rotational Equilibrium  and Dynamics

Conceptual Question…• 1: A student pushes with minimal force of 50.0 N

on the middle of a door to open it.

– What minimum force must be applied at the edge of the door in order for the door to open?

– 25 Newtons – (half a much because the distance in increased by 2)

– T = d * F– What minimum force must be applied to the hinged side

of the door in order for the door to open?– The door cannot be opened by a force at the hinge

location. It can be broken but not opened normally.

Page 11: Rotational Equilibrium  and Dynamics

Torque can be (+) or (-)

• Torque is a vector quantity (i.e. has direction)• To find net torque, simply add up the

individual torques.Tnet = Sum of Torques = T1 + T2 = (F1d1) + (F2d2)

The sign of the net torque value (+ or -) will tell you the direction an object rotates.

Clockwise rotation = - torqueCounterclockwise rotation = + torque

Page 12: Rotational Equilibrium  and Dynamics

Example: Torque

• A basketball is being pushed by two players during tip-off. One player exerts a downward force of 11 N at a distance of 0.07 m from the axis of rotation. The second player applies an upward force of 15 N at a perpendicular distance of 0.014 m from the axis of rotation.

• Find the net torque acting on the basketball.

Page 13: Rotational Equilibrium  and Dynamics

Example: Torque

• A basketball is being pushed by two players during tip-off. One player exerts a downward force of 11 N at a distance of 0.07 m from the axis of rotation. The second player applies an upward force of 15 N at a perpendicular distance of 0.14 m from the axis of rotation.

• Find the net torque acting on the basketball.

Givens: Formula:F1 = 15 N d1 = 0.14 m Tnet = T1 + T2

F2 = 11 N d2 = 0.07 m

Page 14: Rotational Equilibrium  and Dynamics

Example: Torque

• A basketball is being pushed by two players during tip-off. One player exerts a downward force of 11 N at a distance of 0.07 m from the axis of rotation. The second player applies an upward force of 15 N at a perpendicular distance of 0.14 m from the axis of rotation.

• Find the net torque acting on the basketball.

Givens: Formula:F1 = 15 N d1 = 0.14 m Tnet = T1 + T2

F2 = 11 N d2 = 0.07 m

d2 = 0.07 m

F2 = 11 N

d1 = 0.14 m

F1 = 15 N

Page 15: Rotational Equilibrium  and Dynamics

• A basketball is being pushed by two players during tip-off. One player exerts a downward force of 11 N at a distance of 0.07 m from the axis of rotation. The second player applies an upward force of 15 N at a perpendicular distance of 0.14 m from the axis of rotation.

• Find the net torque acting on the basketball. Givens: Formula:F1 = 15 N d1 = 0.14 m Tnet = T1 + T2

F2 = 11 N d2 = 0.07 m

T1 = F1 d1 = -(15)(0.14) = -2.1 Nm

T2 = F2 d2 = -(11) (0.07)= -0.77Nm

(both forces produce a clockwise rotationTherefore both torques are negative)

d2 = 0.07 m

F2 = 11 N

d1 = 0.14 m

F1 = 15 N

Page 16: Rotational Equilibrium  and Dynamics

• A basketball is being pushed by two players during tip-off. One player exerts a downward force of 11 N at a distance of 0.07 m from the axis of rotation. The second player applies an upward force of 15 N at a perpendicular distance of 0.14 m from the axis of rotation.

• Find the net torque acting on the basketball. T1 = F1 d1 = -(15)(0.14) = -2.1 Nm

T2 = F2 d2 = -(11) (0.07)= -0.77Nm

Tnet = T1 + T2 = -2.1 – 0.77

Tnet = -2.9 N mNegative torque thus Ball rotates in a clockwise direction.

d2 = 0.07 m

F2 = 11 N

d1 = 0.14 m

F1 = 15 N

Page 17: Rotational Equilibrium  and Dynamics

Individual Practice

• Take 5 minutes to work the following on your own:*problem 1 (practice 8A) on page 282

Page 18: Rotational Equilibrium  and Dynamics

ROTATION and INERTIA

• Identify Center of Mass• Distinguish between mass and moment of

Inertia• Define the second condition of equilibrium• Solve problems involving the first and second

conditions of equilibrium

Page 19: Rotational Equilibrium  and Dynamics

Center of Mass

• Center of Mass – the point at which all the mass of the body can be considered to be concentrated when analyzing translational motion.

• Consider a stick thrown in the air while playing fetch with a puppy…

Page 20: Rotational Equilibrium  and Dynamics

• Since the center of mass is considered to be the point at which all the mass of an object is concentrated…

• The stick rotates in the air around its center of mass• The complete motion of the stick in the air is both rotational and translational.

The center of mass moves as if the stick were a point mass, with all of its mass concentrated

at that point for purposes of analyzing its translational motion.

Page 21: Rotational Equilibrium  and Dynamics

Moment of Inertia

• Moment of inertia: the tendency of a body rotating about a fixed axis to resist a change in rotational motion.

• The moment of inertia is a measure of the object’s resistance to a change in its rotational motion about some axis.

Page 22: Rotational Equilibrium  and Dynamics

Calculating Moment of Inertia

• Depends of the shape of the object.• SI units: kg x m2

See table 8-1 in textbook for the different formulas.

Page 23: Rotational Equilibrium  and Dynamics

Rotational Equilibrium

• Rotational Equilibrium is different from translational equilibrium– If the net force on an object is zero, then the object

is in translational equilibrium– If the net torque on an object is zero, then the

object is in rotational equilibrium– THUS, for an object to be completely in equilibrium,

the net force and the net torque must be zero– The dependence of equilibrium on the absence of net

torque is called the second condition for equilibrium.

Page 24: Rotational Equilibrium  and Dynamics

ROTATIONAL DYNAMICS

• Describe Newton’s 2nd law for rotation

• Calculate the angular momentum for various rotating objects.

Page 25: Rotational Equilibrium  and Dynamics

Newton’s 2nd Law for Rotation

t net = Net torque = moment of Inertia x angular

acceleration

Remember…for translational motion, F=ma

Page 26: Rotational Equilibrium  and Dynamics

Ex: Newton’s 2nd law for rotation

• A student tosses a dart using only the rotation of her forearm to accelerate the dart. The forearm rotates in a vertical plane about an axis at the elbow joint. The forearm and dart have a combined moment of Inertia of 0.075 kgm2 about the axis, and the length of the forearm is 0.26m. If the dart has a tangential acceleration of 45 m/s2 just before released, what is the net torque on the arm and dart?

Page 27: Rotational Equilibrium  and Dynamics

A student tosses a dart using only the rotation of her forearm to accelerate the dart. The forearm rotates in a vertical plane about an axis at the elbow joint. The forearm and dart have a combined moment of Inertia of 0.075 kgm2 about the axis, and the length of the forearm is 0.26m. If the dart has a tangential acceleration of 45 m/s2 just before released, what is the net torque on the arm and dart?

GIVEN:I= 0.075 kg x m2

a = 45 m/s2

d = 0.26 m = ?

= = (where = a/d)= (a/d)= (0.075)(45/0.26)= 13 Nm

Page 28: Rotational Equilibrium  and Dynamics

MOMENTUM

• Angular Momentum: the product of a rotating object’s moment of inertia and angular speed about the same axis

L = ()

Angular momentum = moment of Inertia x angular speed

Page 29: Rotational Equilibrium  and Dynamics

Conservation of Angular Momentum

• When the net external torque acting on an object or objects is zero, the angular momentum of the object(s) does not change. This is the:

Law of Conservation of Angular Momentum.

Page 30: Rotational Equilibrium  and Dynamics

• Assuming the friction between skates and the ice is negligible, there is no torque acting on an ice skater.

When she brings her hands in and feet closer to her body, more of her mass on average is nearer to her axis of rotation. Thus, the moment of inertia is constant and her angular speed increases to compensate for her smaller moment of inertia.

Page 31: Rotational Equilibrium  and Dynamics

Rotational Kinetic Energy

• Rotational KE = ½ x moment of Inertia x angular speed 2

KErot = ½ 2

Rotational KE = energy of an object due to its rotational motion

Rotational KE is conserved in the absence of any external force moving an

object.

Page 32: Rotational Equilibrium  and Dynamics

Be ready for a vocab quiz on Friday

• Torque Work • Lever Arm Energy• Center of Mass Momentum• Moment of Inertia Angular Speed• Angular Momentum Angular Acceleration• Rotational Kinetic Energy Rotational Motion• 6 types of simple machines “SAWLIP”