# 6.1 Force and Newton's Laws ```Force and Newton’s Laws
Insert Gif of box being pushed in different dimensions
1.1
Different types of forces:
Every student attempting the Senior Certificate Exam for Physical Sciences should learn all the
definitions as given in the Exam guidelines of 2017. It is important to know that a force can be a
push, a pull or it can be a force in a rope (tension). Because most examples in this section is
linked to a sketch, it is also important to know all the SI-units for each force.
•
•
Normal force (N) is the force or component of the exerted force by the surface an object
rests on. The force is exerted perpendicular to the surface.
Friction (f) is the force that resists the movement of an object and is always parallel to
the surface. It is important to differentiate with symbols between static- and kinetic
friction.
o Static friction (fs) is the force resisting the tendency of an object at rest to start
moving relative to the surface.
It is much more difficult to get an object moving and breaking loose from the
surface it is resting on than to keep a moving object in motion. For this reason
the maximum static friction on an object is always bigger than the kinetic friction
of the two surfaces on each other. (This is true at the point where an object
breaks loose from the surface in order to start moving.)
o
o
o
o
o
Kinetic friction (fk) is the force resisting the movement of a moving object relative
to the surface it moves on.
Friction forces is always:
▪ proportional to the normal force
▪ independent of the contact surface (This implies that a brick on a
concrete floor will experience the same friction irrespective of the way it is
positioned...
▪ independent of the velocity of the moving object.
If a force, F, exerted parallel to the surface, does not cause the object to move, it
will mean that the magnitude of that force is equal in magnitude to the static
friction force.
The static friction force is at a maximum (fsmax) at the moment the object starts to
break loose from the surface to move.
If the applied force is bigger than fsmax, the resultant/ net force will cause the
object to accelerate.
1.2
The following formulas can be used for questions on forces and Newton’s Laws on the
formula page:
Fnet = ma
fsmaks = &micro;s N
F=G
1.3
fk = &micro;kN
m1 m2
g=G
d2
M
d2
Force diagrams and free body diagrams
It is recommended that you ALWAYS draw a small force diagram for physics questions
involving forces, even if it is not requested. A force diagram uses a box to represent a body’s
centre of mass. Vector arrows are then drawn from the box with relative magnitudes and
directions that are isolated in the area of the object.
A free-body diagram only uses a dot in the centre of the represented object for the centre of
mass.
Because all equations are only applicable in ONE dimension, it is sometimes necessary to
break two-dimensional forces (for example a force forming an angle with the horizontal or an
object pussing down on an inclined plane) into it’s two components. It is important though to
remember that a sketch drawn for marks in the paper must ONLY consist of EITHER the main
force or the components of the force, not both on the same force diagram. By making the
mistake of drawing both, your vectors represent a vector of double the magnitude.
The force diagrams enables you, with the necessary background, to calculate the net/ resultant
forces.
1.4
Example 1.
Force diagrams:
1.4.1
Exemplar 2014 Question 2
Draw a labeled free-body diagram of all the forces working in on the 6kg-block as it moves up
the inclined plane.
Example 1.4.2: November 2015 Question 2
Draw a labeled force diagram for both blok M and the 2,5 kg- block.
Example 1.4.3 DBE Feb/Mrt 2018 Question 2
Draw a fully labeled free body diagram for Block Q.
Solution 1.4.1 DBE Exemplar 2014 Question 2
Solution 1.4.2 DBE November 2015 Question 2 Adapted
Solution 1.4.3 DBE Feb/Mrt 2018 Question 2
1.5
Example 1.5.1 DBE Feb 2017 Question 2
Solution 1.5.1 DBE Feb 2017 Question 2
2.1
2.2
2.3.1
2.3.2
Zero
See to it that every force has
a label with the name written
down below, next to the
symbol. Unnecessary marks
will be forfeited if the forces
are not labeled.
2.3.3
This particular part of the
learners only, but all the
previous questions is on
chapter forms part of the
2.
Only in the grade 11 curriculum does scale drawings form part of the required set of skills. The
reason behind this chapter in the work is that some concepts on vectors are understood more
easily if you draw a sketch thereof. The sketching brings about inside knowledge of certain
techniques, that would otherwise be neglected. Many people believe that technology already
replaced hand-drawn sketches, but many technical problems in programming cannot be
corrected without a proper knowledge of the background of the problem. In this section we look
at drawings that will be done with a protractor, pencil and a ruler:
•
Draw a sketch of the vertical vectors (y-axis) and horizontal vectors (x-axis) on a
Cartesian plane. This involves one dimensional vectors that will fit exactly on the vertical
or horizontal axes of the Cartesian plane. For example:
8
6
F1:6N North
4
2
10
5
5
10
15
20
F2: 5N East
2
4
6
•
Add co-linear vertical vectors and co-linear horizontal vectors together to find the net
vertical vector (Ry) and the net horizontal vector (Rx). (Co-linear vectors refers to vectors
in a straight line). In this example it is still about vectors in the same dimension. For
example:
8
6
4
2
10
5
5
10
15
20
2
4
6
•
Solution:
Horizontal – Right/ East as positive Rx = 6 +7 -8 = 5 Units East/right
Vertical – Upwards/North as positive Ry = -6 + (-3) = -9 of 9 Units downward/ South
Sketch the resultant (R) by using the head-to-tail or tail-to-tail method.
2.1
This method draws the vectors as vector arrows following one another. The following
vector will be drawn where the previous one ends. The magnitude (and thus the length
of the arrow) is of great importance and therefor it is also important to write down the
scale used for the drawing. For example 1cm:10m or what ever will be convenient for
the magnitude of force vectors you are working with. (Remember that it is not only
forces that can be drawn according to these methods, but any other vector as well.) The
past few years a scale was provided according to which the drawings had to be done.
The head-to-tail method can be used for an unlimited number of vectors, where the
resultant will be drawn connecting the start of the FIRST vector, in a straight line with the
end of the LAST vector. Measure the angle of the resultant to determine the direction of
the resultant vector. The length of the resultant vector should firstly be measured and
then converted by means of the scale that was used to see exactly how big the vector
really is.
2.2
Tail-by-tail method:
This method can only be used for TWO vectors to determine the resultant. That tail-bytail method forms a parallelogram with the two vectors as the two sets of parallel sides of
the parallelogram from the same corner. The resultant will be the diagonal starting from
the same corner as the other two vectors (all tails of the vector angles together) to the
opposite corner of the parallelogram. The two vectors of which the resultant needs to be
calculated is drawn in the same Cartesian plane. Measure carefully to draw the
remaining two sides of a parallelogram with each opposite side equal. The length and
direction of the diagonal line that is ALSO drawn from the same starting point in the
same Cartesian plane will be the values for the Resultant. The length again as in the
previous method needs to be converted by the scale that was used to draw the sketch.
Please make sure whether the question says that you have to determine a resultant
vector (may include up to four vectors in one or in two dimensions) GRAPHICALLY or if
it should be CALCULATED.
Through calculation it will be necessary to use the Pythagoras theory, the Sinus-rule in
mathematics or easy trigonometry functions.
A closed vector diagram shows that the forces acting on an object are in equilibrium.
This means the net resultant on the object is equal to zero as in Newton’s first law. The
object on which the forces in equilibrium is exerted will either stay at rest OR continue
movement at a constant velocity. If there are three forces involved, the forces can be
rearranged to form a closed triangle where other mathematical principles can be applied.
This type of questions can include calculating the breaking tension of a rope or
calculating which rope carries the most tension. Look at the following examples from
GDE question papers:
2.3 Example
June 2014
1.1
Three objects A, B and C is hanging from a rope that has a knot at O, as
indicated in the diagram below:
O
F3
F2
F1
Which vector diagram best represents the relation between the forces exerted
through point O?
F3
A.
F3
B.
F1
F1
1.2
F3
D.
F1
F1
F2
F2
F3
C.
F2
F2
D
The figure below represents a book on a table. Two forces are exerted on the
book. According to Newton’s third law, the reaction force of F will be...
F
A.
B.
C.
D.
the gravitational force of the earth exerted on the book.
the force of the table on the earth.
the force of the table on the book.
the force of the book on the table.
1.3
C (F is the force of the book on the table)
A vehicle moves horizontally at a constant velocity of 60 km∙h-1.
Which ONE of the force diagrams below correctly represents the forces acting in on the
car?
A.
B.
C.
D.
D
Question 2
2.
An 8 kg mass is hanged from the roof by a rope. A second rope pulls the mass in a
horizontal direction as shown in the diagram below. Calculate the tension in each of the
ropes.
(g=9,8 m∙s-2)
T1
30&deg;
Ring in equilibrium
8kg
T2
W= mg = 78,4 N
2.1
Draw a vector diagram to show that forces T1, T2 and W is in equilibrium.
(3)
2.2
Determine the value of the forces T1 and T2.
(6)
2.1
30&deg;
T1
W=78,4 N
60&deg;
T2
2.2
Fg = ma
= 8x9,8
=78,4 N
W
cos 30&deg; =T
1
T1 = 90,52 N
tan 30&deg; =
T2
W
T2 = 45,26 N
November 2014
3.
The diagram below shows a rope-and-pulley system used lift an 800 N -object from the
ground. Accept that the ropes are almost weightless and unelastic and that the pulleys
are light and frictionless.
T2
Pulley P
T1
140&deg; 120&deg;
800 N
Calculate the:
3.1
Magnitude of the tension in T1 and T2 graphically.
(7)
3.2
Magnitude and direction of the reaction force at pulley P.
(4)
3.1
3.2
3
Newton’s first, second and third laws:
Colorado... A force that is exerted horizontally, can be much smaller than the weight of
an object, depending on the magnitude of the friction force:
NEWTON I: A body will remain in its state of motion (at rest or moving at constant velocity) until
a net force acts on it.
NEWTON II: When a net force acts on an object, the object will accelerate in the direction of
the net force and the acceleration is directly proportional to the force and inversely proportional
to the mass of the object.
NEWTON III: When one body exerts a force on a second body, the second body exerts a force
of equal magnitude in the opposite direction on the first body.
NEWTONS UNIVERSAL GRAVITATIONAL LAW: Each body in the universe attracts every
other body with a force that is directly proportional to the product of their masses and inversely
proportional to the square of the distance between their centres.
3.1
Application:
Each of the above laws can be applied in real-life situations. What is important in the answering
of the questions is to choose ONE direction as positive to calculate the other forces. Vertical
and diagonal forces cannot be calculated together in the same equation. The force making an
angle with the horizontal should rather be broken down to its’ components and then only take
the direction you are working with into account.
Calculations with Newton’s Laws can be applied to objects in rest as well as moving objects.
The symbols used all refers back to:
Fnet = ma
The net force of the system can be zero, when the forces in the system is in equilibrium as
stated in Newton 1(Equilibrium problems). Equilibrium allows an object to have a certain
velocity, as Newton 1 explains that if the net force working in on the object is zero, the velocity
will remain constant. In such cases you can also substitute a zero into the acceleration
placeholder, a.
The other scenario is that there is a non-zero net force as is the case with the other laws (Nonequilibrium problems). This means there will be an acceleration. It is here where the Grade 10
horizontal laws of motion also comes in handy and must sometimes be applied. Remember that
the Senior Certificate Exam includes this Grade 10 chapter. The Newton Laws can be applied
in the following situations:
•
A single object:
o Moving on a horizontal plane with or without friction
o Moving on an inclined plane with and without friction
o Moving in the vertical plane (lifts, rockets, etc.)
•
Two-body systems (joined by a light inextensible string):
o Both on a flat horizontal plane with and without friction
o One on a horizontal plane with and without friction, and a second hanging
vertically from a string over a frictionless pulley
o Both on an inclined plane with or without friction
o Both hanging vertically from a string over a frictionless pulley
Look at the following example that is addapted for Grade 11 learners:
3.2
Example 3.3: DBE November 2015 Question 2
Solution 3.3: DBE November 2015 Question 2
4
Breakdown of diagonal forces:
It is important to know how to handle a two-body system as in the example above.
The two blocks M and the 2,5 kg block moves together as a system, even though the 2,5 kg
block moves vertical and block M moves horizontally. It is therefore also important to choose
one direction as positive before any substitutions is made into some formulas. This kind of
problems are solved by simultaneous equations. If you choose the DOWNWARD movement of
the 2,5 kg block as positive, then the RIGHT direction of block M should also be positive to keep
the systems vectors positive in the same direction. It may happen that the friction of block M is
bigger than the tension in the rope between the blocks, which will result in a zero acceleration or
a negative answer for some of the vectors. That information is important at the end of solving
the equations in order to apply the right directions for the system...
Continue the rest of the sub-questions by still applying the positive directions for certain
directions...
As a result, it is also important to break down forces working on an incline into parallel and
perpendicular components in order that there is still only one direction as positive when
4.1
Step 1:
Draw all the forces involved on your sketch and also indicate the degree of the inclined plane.
FN
f
Fg
30&deg;
Take care that you always draw the free-body diagram like the diagram above, if it is needed as
part of a sub-question, but ALSO a key below it with the key as well as the name of each force,
for example:
FN: Normal force
Fg: Gravitational force
f: Friction force
BUT on your own answer sheet you ALWAYS need to draw a free-body diagram for each object
and that would be the drawing where you can “color” the picture as you need to help you with
calculations. Write as much information on it as you possibly can. This will help you also with
4.2
Step 2:
Extend the normal force to cut through the inclined plane. This line is supposed to be
perpendicular to the incline of the plane!!
FN
Fg
30&deg;
30&deg;
Now the red newly added line will represent Fg┴. The angle between the extension of the
normal force and Fg will be the same as the angle of the incline of the plane. Write it on your
sketch!!! This will enable you to determine the trigonometry relation of the red side of the
triangle that is formed. See the last step to ensure that the triangle is drawn correctly...
4.3
Step 3:
Complete the last side of the right angled triangle by drawing one last dashed line, forming a
right angle (90 degrees) with the red line. This blue line represents the parallel component of
weight Fgll.
Substituting the different forces into an equation is not as much of a problem as learners
struggle to apply their trigonometry knowledge. Assure that you break down the forces of each
Newton question into its’ components and only substitute forces in ONE dimension into each
equation.
5.
Newton’s Universal Gravitational Law
Newtons’ Universal Law:
Each body in the universe attracts every other body with a force
that is directly proportional to the product of their masses and inversely proportional to the
square of the distance between their centres.
Weight is the gravitational force exerted by the earth on any object on or near it’s surface.
m1 m2
r2
F=G
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