Force:- Any pull or push”, unit: kg met/sec2 or Newton (N)
Types of forces:-
1- Field Forces:- No need of contact
Always attraction type
Direction:- Always along (-y) axis or straight vertically down ward.
(2). Contact forces: There must be some contact
(i) Normal force (N):- This force act when two surfaces of different object are in contact.
Direction:- perpendicular to contact surfaces.
(ii). Frictional force(f):- This force also act when two surfaces of different objects in contacts.
Direction:- Parallel to contact surfaces
Also F = m N here m is coefficient of friction.
Now
N → Perpendicular to contact surface
So F ^ N
Understanding of frictional force
The force which resist the motion”
mS > mk m can be less than or greater than one
If Fext = 0, f = 0
Example:- 1
Now
fs = msN
= ms mg
= 0.6 x 10 x 10
fs = 60 N
fk = mkN
= 0.2 x 10 x10
fk = 20 N
Amount of frictional force = 0
Because fext = 0, = f = 0
Example:- 2
m = 10 kg As in case (i) fs = 60 N, fk = 20 N
f = fs = 40 N
Body is at rest
Example:- 3
As in case (i) fs = 60N, fk = 20 N
f = fs = 60 = Fext → limitation friction
Body is at rest but tends to move
Example:- 4
As in case = fs = 60N, fk = 20N
Body is in moving condition
10a = 85 - 20
f = fk = 20 N
(3) Attachment forces indirect force
Direction: Direction of tension (T) is always away from the body.
Example:-
10 g –T = 10 a ---- (1)
N = 5 g ------(2)
T = 5a --------(3)
Solving 1& 310 g - 5a = 10a
15a = 10g
T = 5a
Net force on the pulley
Example:-
fs = ms N
= 0.5 x 5g
fs = 25 N
fk = mk N
= 0.2 x 5g
fk = 10 N
Pulling force for 5 kg
10 g = 100 N
So both block will move
10 g –T = 10a -----(1)
T -mkN = 5a ------(2)
T – 10 = 5a
N = 5g -----(3)
Solving (1) & (2)
10g –T = 10a
1-10 = 5a
90 = 15a Þ2
Similarly
T -10 = 5 x 6 T= 40N
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