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PHYSICS LowerSixth science

CHAPTER 4 LAWS OF MOTION

VIII. MOTION ON AN INCLINED PLANE

When an object moves along an inclined plane then: different forces act on it like normal

reaction of plane, friction force acting in opposite direction of motion etc. Different relations

for the motion are given below.

Normal reaction of plane

R = mg cos θ

and net force acting downward on the block.

F = mg sin θ – f

Acceleration on inclined plane a = g (sin θ – μ cos θ)

When angle of inclination of the plane from horizontal is less than the angle of repose (α), then

  • minimum force required to move the body up the inclined plane

                               f1 = mg (sin θ + μ cos θ)

  • minimum force required to push the body down the inclined plane

                               f2 = mg (μ cos θ – sin θ) J

Tension

Tension force always pulls a body. Tension is a reactive force. It is not an active force.

Tension across a massless pulley or frictionless pulley remain constant. Rope becomes slack when tension force becomes zero.

Motion of Bodies in Contact

  • Two Bodies in Contact If F force is a applied on object of mass m1 then acceleration of the bodies

a = F / (m1 + m2)

Contact force on m1 = m1 a = m1F / (m1 + m2)

Contact force on m2 = m2 a = m2 F / (m1 + m2)

Three Bodies in Contact If F force is applied an object of mass m1, then acceleration of the bodies = F / (m1 + m2 + m3)


Contact force between m1 and m3

F1 = (m1 + m3) F / (m1 + m2 + m3)

Contact force between m2 and m3

F2 = m3 F / (m1 + m2 + m3)

Motion of Two Bodies, One Resting on the Other

  1. The coefficient of friction between surface of A and B be μ. If a force F is applied on the lower body A. then common acceleration of two bodies


a = F / (M + m)

Pseudo force acting on block B due to the accelerated motion

f’= ma

The pseudo force tends to produce a relative motion between bodies A and B and consequently a frictional force

f = μ N = μmg is developed. For equilibrium

ma ≤ μ mg or a ≤ μg

  1. Let friction is also present between the ground surface and body A Let the coefficient of friction between the given surface and body A is μ1 and the coefficient of friction between the surfaces of bodies A and B is μ2 If a force F is applied on the lower body A


Net accelerating force = F – fA = F – μ1(M + m)g

 Net acceleration

a = F – μ1 (M + m)g / (M + m) = F / (M + m) – μ g

Pseudo force acting on the block B

f’ = ma

The pseudo force tends to produce a relative motion between the bodies A and B are

Consequently a frictional force fB = μ mg is developed. For equilibrium

ma-le; μ2 mg or a ≤ μ2 g

If acceleration produced under the effect of force F is more than μ2g, then two bodies will not move together.

 Motion of Bodies Connected by Strings

Acceleration of the system a = F / (m1 + m2 + m3)

Tension in string T1 = F

T2 = (m2 + m3) a = (m2 + m3) F / (m1 + m2 + m3)

T3 = m3a = m3F / (m1 + m2 + m3)

Pulley Mass System

  • When unequal masses m1 and m2 are suspended from a pulley

(m1 > m2)

m1 g – T = m1 a, and T – m2 g = m2 a

On solving equations, we get

a = ((m1 – m2) / (m1 + m2)) * g

T = 2 m1m2  / (m1 + m2) * g


  • When a body of mass m1 is placed frictionless horizontal surface, then

                 

Acceleration a = m1 g / (m1 + m2)

Tension in string T = m1 m2 g / (m1 + m2)

  • When a body of mass m2 is placed on a rough horizontal surface, then


Acceleration a = ((m1 – μm2) / (m1 + m2)) * g

Tension in string T = (m1 m2(1 + μ) / (m1 + m2)) * g

  • When two masses m1 and m2 are connected to a single mass M as shown in figure, then
  • m1 g – T1 = m1 a …..(i)

    T2 – m2 g = m2 a ……(ii)

    T1 – T2 = Ma …….(iii)

    Acceleration a = ((m1 – m2 / (m1 + m2 + M)) * g

    Tension T1 = (2m2 + M / (m1 + m2 + M) * m1 g

    T2 = (2ma + M / (m1 + m2 + M) * m2 g

  • Motion on a smooth inclined plane, then

m1g – T = m1a …..(i)

T – m2 g sin θ = m2 a ……(ii)

Acceleration a = ((m1 – m2 sin θ/ (m1 + m2)) * g

Tension T = m1 m2 (1 + sin θ) g / (m1 + m2)

  • Motion of two bodies placed on two inclined planes having different angle of inclination,

Then

Acceleration a = (m1 sin θ1 – m2 sin θ2) g / m1 + m2

Tension T = (m1 m2 / m1 + m2) * (sin θ1 – sin θ2) g

 

EXERCICE:

Multiple choice

  1. Figure 1A shows three force vectors. Which of the vectors A.B.C.D.E in figure 1A would be most to represent their resultant?


 

 

 

 

par Claude Foumtum


PHYSICS LowerSixth science



CHAPTER 2 MOTION IN A STRAIGHT LINE