What is Weight in Physics | Definition, Example – Laws of Motion

What is Weight in Physics | Definition, Example – Laws of Motion

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Weight Definition Physics (w):
It is a field force. It is the force with which a body is pulled towards the centre of the earth due to gravity. It has the magnitude mg, where m is the mass of the body and g is the acceleration due to gravity.

w = mg

Normal Reaction
It is a contact force. It is the force between two surfaces in contact, which is always perpendicular to the surfaces in contact.

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 remains constant.
  • Rope becomes slack when tension force becomes zero.

Apparent Weight in Lift
(i) When a lift is at rest or moving with a constant speed, then
Weight

The weighing machine will read the actual weight.

(ii) When a lift is accelerating upwards, then apparent weight

R1 = m(g + a)

Weight
The weighing machine will read the apparent weight, which is more than the actual weight.

(iii) When a lift is accelerating downwards, then apparent weight

R2 = m(g-a)

Weight
The weighing machine will read the apparent weight, which is less than the actual weight.

(iv) When lift is falling freely under gravity, then

R2 = m(g-g) = 0

The apparent weight of the body becomes zero.

(v) If lift is accelerating downward with an acceleration greater than g, then body will be lifted from floor to the ceiling of the lift.

Laws of Motion:
There are various laws in Physics that define the motion of the object. When an object is in motion whether it is linear or circular there is some force which is always imposed on it.

What is Inertia of Motion Force
Law of Conservation of Linear Momentum Impulse
Laws of Motion Rocket
Equilibrium of a Particle Weight
Friction Motion on a Rough Inclined Plane
Motion of Bodies in Contact Pulley Mass System

Motion on a Rough Inclined Plane | Definition, Example – Laws of Motion

Motion on a Rough Inclined Plane | Definition, Example – Laws of Motion

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Motion of a body on a Rough 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
Motion on a Rough Inclined Plane

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
(i) minimum force required to move the body up the inclined plane

F1 = mg (sin θ + μ cos θ)

(ii) minimum force required to push the body down the inclined plane

F2 = mg (μ cos θ – sin θ)

Laws of Motion:
There are various laws in Physics that define the motion of the object. When an object is in motion whether it is linear or circular there is some force which is always imposed on it.

What is Inertia of Motion Force
Law of Conservation of Linear Momentum Impulse
Laws of Motion Rocket
Equilibrium of a Particle Weight
Friction Motion on a Rough Inclined Plane
Motion of Bodies in Contact Pulley Mass System

Motion of Bodies in Contact | Definition, Types – Laws of Motion

Motion of Bodies in Contact | Definition, Types – Laws of Motion

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Motion of Bodies in Contact
1. Contact Force Between Two Blocks:
If force F is applied on an object of mass m1, then acceleration of the bodies
Motion of Bodies in Contact
Contact force on m1 = m1a = \(\frac{m_{1} F}{\left(m_{1}+m_{2}\right)}\)
Contact force on m2 = m2a = \(\frac{m_{2} F}{\left(m_{1}+m_{2}\right)}\)

2. Contact Force Between Three Blocks:
If force F is applied on an object of mass m1, then acceleration of the bodies
= \(\frac{F}{\left(m_{1}+m_{2}+m_{3}\right)}\)
Motion of Bodies in Contact
Contact force between m1 and m2
\(F_{1}=\frac{\left(m_{2}+m_{3}\right) F}{\left(m_{1}+m_{2}+m_{3}\right)}\)
Contact force between m2 and m3
\(F_{2}=\frac{m_{3} F}{\left(m_{1}+m_{2}+m_{3}\right)}\)

3. Motion of Two Bodies One Resting on the Other:
(a) 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
Motion of Bodies in Contact
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 ≤ μmg or a ≤ μg

(b) 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.
Motion of Bodies in Contact

Net accelerating force F – fA = F – μ1 (M + m)g
∴ Net acceleration
\(a=\frac{F-\mu_{1}(M+m) g}{(M+m)}=\frac{F}{(M+m)}-\mu_{1} g\)

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 = μ2 mg is developed. For equilibrium
ma ≤ μ2mg or a ≤ μ2g
If acceleration produced under the the effect of force Fis more than μ2g, then two bodies will not move together.

4. Motion of Bodies Connected by a String:
Motion of Bodies in Contact

Acceleration of the system a = \(\frac{F}{\left(m_{1}+m_{2}+m_{3}\right)}\)
Tension in string
T1 = F
T2 = (m2 + m3) a = \(\frac{\left(m_{2}+m_{3}\right) F}{\left(m_{1}+m_{2}+m_{3}\right)}\)
T3 = m3a = \(\frac{m_{3} F}{\left(m_{1}+m_{2}+m_{3}\right)}\)

Laws of Motion:
There are various laws in Physics that define the motion of the object. When an object is in motion whether it is linear or circular there is some force which is always imposed on it.

What is Inertia of Motion Force
Law of Conservation of Linear Momentum Impulse
Laws of Motion Rocket
Equilibrium of a Particle Weight
Friction Motion on a Rough Inclined Plane
Motion of Bodies in Contact Pulley Mass System

What is Friction in Physics? | Definition, Examples, Types of Friction – Laws of Motion

Friction Definition Physics:
A force acting on the point of contact of the objects, which opposes the relative motion is called friction.

What is Friction in Physics? | Definition, Examples, Types of Friction – Laws of Motion

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  • It acts parallel to the contact surfaces.
  • Frictional forces are produced due to intermolecular interactions acting between the molecules of the bodies in contact.

Types of Friction:

  1. Static Friction
  2. Limiting Friction
  3. Kinetic Friction

1. Static Friction Definition:
It is an opposing force which comes into play when one body tends to move over the surface of the other body but actual motion is not taking place.

Static friction is a self-adjusting force which increases as the applied force is increased. Static friction opposes impending motion.

2. Limiting Friction Definition:
It is the maximum value of static friction when body is at the verge of starting motion.

Limiting friction, fs(max) = μlR

where, μl = coefficient of limiting friction and R = normal reaction.
Limiting friction do not depend on area of contact surfaces but depends on their nature, i.e. smoothness or roughness.
Friction

Angle of Friction Definition:
It is the angle which the resultant of the force of limiting friction and the normal reaction(N) makes with the direction of N.

μl = tan θ

Angle of Repose in Friction or Angle of Sliding
It is the minimum angle of inclination of a plane with the horizontal, such that a body placed on it, just begins to slide down.
If angle of repose is a and coefficient of limiting friction is μl, then

μl = tan α

3. Kinetic Friction Definition:
It is an opposing force that comes into existence when one object is actually moving over the surface of other object.
Friction

Kinetic friction (fk) = μk R

where, μk = coefficient of kinetic friction and R = normal reaction.

Kinetic friction is of two types:
(a) Sliding friction
(b) Rolling friction
As, rolling friction < sliding friction, therefore it is easier to roll a body than to slide.

Laws of Motion:
There are various laws in Physics that define the motion of the object. When an object is in motion whether it is linear or circular there is some force which is always imposed on it.

What is Inertia of Motion Force
Law of Conservation of Linear Momentum Impulse
Laws of Motion Rocket
Equilibrium of a Particle Weight
Friction Motion on a Rough Inclined Plane
Motion of Bodies in Contact Pulley Mass System

Newton’s Laws of Motion | Definition, Examples – First, Second and Third law – Laws of Motion

Newton’s Laws of Motion Definition:
Newton’s laws of motion explains the linear momentum and moment of inertia of moving objects.

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Newton’s Laws of Motion | Definition, Examples – First, Second and Third law – Laws of Motion

1. Newton’s First Law of Motion Definition:
A body continues to be in its state of rest or in uniform motion along a straight line unless an external force is applied on it. Newton’s First Law of Motion is also known as law of inertia.

Newton’s First Law of Motion Examples

  • When a carpet or a blanket is beaten with a stick, then the dust particles separate out from it.
  • If a moving vehicle suddenly stops, then the passengers inside the vehicle bend outward.

2. Newton’s Second Law of Motion:
Newton’s Second Law of Motion gives us the rate of change of linear momentum is proportional to the applied force and change in momentum takes place in the direction of applied force.

Newton’s Second Law of Motion Mathematical Expression is,

F α \(\frac{d \mathbf{p}}{d t}\) ⇒ F = k \(\frac{d}{d t}\)(mv)

where, k is a constant of proportionality and its value is one in SI and CGS system.

F = \(\frac{m d \mathbf{v}}{d t}\) = ma

The second law of motion is a vector law. It is equivalent to three equations. One for each component of the vectors.

Laws of Motion

Newton’s Second Law of Motion Examples

1. It is easier for a strong adult to push a full shopping cart than it is for a baby to push the same cart (this is depending on the net force acting on the object).

2. It is easier for a person to push an empty shopping cart than a full one (this is depending on the mass of the object).

3. Newton’s Third Law of Motion Definition:
For every action there is an equal and opposite reaction and both acts on two different bodies.

Laws of Motion

Newton’s Third Law of Motion mathematical formula, F12 = – F21
Newton’s Third Law of Motion Examples

  1. Swimming becomes possible because of third law of motion.
  2. Jumping of a man from a boat onto the bank of a river.
  3. Jerk is produced in a gun when bullet is fired from it.
  4. Pulling of cart by a horse.

Note:
Newton’s second law of motion is called real law of motion because first and third laws of motion can be obtained from it.

The modern version of these laws are as follows
(i) A body continues in its initial state of rest or motion with uniform velocity unless an unbalanced external force is acted on it.
(ii) Forces always occur in pairs. If body A exerts a force on body B, an equal but opposite force is exerted by body B on body A.

Laws of Motion:
There are various laws in Physics that define the motion of the object. When an object is in motion whether it is linear or circular there is some force which is always imposed on it.

What is Inertia of Motion Force
Law of Conservation of Linear Momentum Impulse
Laws of Motion Rocket
Equilibrium of a Particle Weight
Friction Motion on a Rough Inclined Plane
Motion of Bodies in Contact Pulley Mass System

Motion in Vertical Circle | Physics – Motion in a Plane

Motion in Vertical Circle | Physics – Motion in a Plane

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Motion of a Particle in a Vertical Circle
(i) Minimum value of velocity at the highest point (i.e. at point C) is \(\sqrt{g r}\)
(ii) The minimum velocity at the bottom required to complete the circle, i.e. at point A
Motion in Vertical Circle
(iii) Velocity of the body when string is in horizontal position, i.e. at point B.
vB = \(\sqrt{3 g r}\)

(iv) Tension in the string
At the top, Tc = 0, At the bottom, TA= 6 mg
When string is horizontal, TB= 3 mg
(i) When a vehicle is moving over a convex bridge, then at the maximum height, reaction (N1) is

N1 = \(m g-\frac{m v^{2}}{r}\)

Motion in Vertical Circle

(ii) When a vehicle is moving over a concave bridge, then at the lowest point, reaction (N2)
Motion in Vertical Circle

N2 = \(m g+\frac{m v^{2}}{r}\)

(iii) When a car takes a turn, sometimes it overturns. During the overturning, it is the inner wheel which leaves the ground first.

Motion in a Plane (Projectile and Circular Motion):
In this chapter or under this topic, we are going to come across the motion of the object when it is thrown from one end to another end. This practice is said to be projection. Also, when an object is moved in a circular motion, then the equation of the motion is derived here. We will learn here about centripetal force and centripetal acceleration in detail with formulas. Also learn the force applied in everyday life motion of the particle in a vertical circle.

Motion in a Plane Projectile Motion
Circular Motion Centripetal Acceleration
Centripetal and Centrifugal Force Examples of Centripetal Force in Everyday Life
Motion in Vertical Circle

Examples of Centripetal Force in Everyday Life – Motion in a Plane

Examples of Centripetal Force in Everyday Life – Motion in a Plane

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Centripetal Force Examples in Real Life

Circular Turning of Roads:
If centripetal force is obtained only by the force of friction between the tyres of the vehicle and road, then for a safe turn, the coefficient of friction (ug) between the road and tyres should be
\(\mu_{s} \geq \frac{v^{2}}{r g} \text { or } \quad v \leq \sqrt{\mu_{s} r g}\)
where, v is the velocity of the vehicle and r is the radius of the circular path.
Maximum velocity for no skidding or slipping is vmax = \(\sqrt{\mu r g}\)
If centripetal force is obtained only by the banking of roads, then the speed (v) of the vehicle for a safe turn
\(v=\sqrt{r g \tan \theta}\)

If speed of the vehicle is less than \(\sqrt{r g \tan \theta}\), then it will move inward (down) and r will decrease and if speed is more than \(\sqrt{r g \tan \theta}\), then it will move outward (up) and r will increase.

In normal life, the centripetal force is obtained by the friction force between the road and tyres as well as by the banking of the roads.

Therefore, the maximum permissible speed for the vehicle is much greater than the optimum value of the speed on a banked road.

When centripetal force is obtained from friction force as well as banking of roads, then maximum safe value of speed of vehicle
\(v_{\max }=\sqrt{\frac{r g\left(\tan \theta+\mu_{s}\right)}{\left(1-\mu_{s} \tan \theta\right)}}\)

Bending of Cyclist:
When a cyclist takes turn at road, he inclines himself from the vertical, slows down his speed and moves on a circular path of larger radius.
If a cyclist is inclined at an angle θ, then tan θ = \(\frac{v^{2}}{r g}\)
where,
v = speed of the cyclist
r = radius of path and g = acceleration due to gravity.

Conical Pendulum Time Period:
It consists of a string OA whose upper-end O is fixed and bob is tied at the other free end. The string is whirled in a horizontal circle, then the arrangement is called a conical pendulum.
Centripetal and Centrifugal Force
Angular speed, ω = \(\frac{v}{r}=\sqrt{\frac{g \tan \theta}{r}}\)
Time period of conical pendulum, T = \(2 \pi \sqrt{\frac{l \cos \theta}{g}}\)

Death Well or Rotor:
In this, a person drives a bicycle on a vertical surface of large wooden well, while in case of a rotor at a certain angular speed of rotor a person hangs resting against the wall without any support from the bottom.
In both the cases, Safe speed, v = \(\sqrt{\frac{g r}{\mu}}\)

Motion in a Plane (Projectile and Circular Motion):
In this chapter or under this topic, we are going to come across the motion of the object when it is thrown from one end to another end. This practice is said to be projection. Also, when an object is moved in a circular motion, then the equation of the motion is derived here. We will learn here about centripetal force and centripetal acceleration in detail with formulas. Also learn the force applied in everyday life motion of the particle in a vertical circle.

Motion in a Plane Projectile Motion
Circular Motion Centripetal Acceleration
Centripetal and Centrifugal Force Examples of Centripetal Force in Everyday Life
Motion in Vertical Circle

Centripetal Force and Centrifugal Force | Definition, Examples, Formulas – Motion in a Plane

Centripetal Force Definition:
It is that force which comes in to play when a body moves on a circular path. It is directed along radius of the circle towards its centre.

Centripetal Force and Centrifugal Force | Definition, Examples, Formulas – Motion in a Plane

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Centripetal Force Formula:
Centripetal force, F = \(\frac{m v^{2}}{r}\) = mrω²
where, m = mass of the body,
v = linear velocity,
ω = angular velocity and r = radius.
Work done by the centripetal force is zero because the centripetal force and displacement are at right angles to each other.

Examples of some incidents and the cause of centripetal force involved.

Incidents

Force Providing Centripetal Force

Orbital motion of planets. Gravitational force between planet and sun.
Orbital motion of electron. Electrostatic force between electron and nucleus.
Turning of vehicles at turn. Frictional force acting between tyres of vehicle and road.
Motion of a stone in circular path, tied with a string. Tension in the string.

Centrifugal Force Definition:
It is defined as the radially directed outward force acting on a body in circular motion as observed by the person moving with the body. It is equal in magnitude but opposite in direction to centripetal force.
Centripetal and Centrifugal Force
Centrifugal force does not act on the body in an inertial frame but arises as pseudo forces in non-inertial frames.

Motion in a Plane (Projectile and Circular Motion):
In this chapter or under this topic, we are going to come across the motion of the object when it is thrown from one end to another end. This practice is said to be projection. Also, when an object is moved in a circular motion, then the equation of the motion is derived here. We will learn here about centripetal force and centripetal acceleration in detail with formulas. Also learn the force applied in everyday life motion of the particle in a vertical circle.

Motion in a Plane Projectile Motion
Circular Motion Centripetal Acceleration
Centripetal and Centrifugal Force Examples of Centripetal Force in Everyday Life
Motion in Vertical Circle

Centripetal Acceleration | Definition, Formula, Units – Motion in a Plane

Centripetal Acceleration | Definition, Formula, Units – Motion in a Plane

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Centripetal Acceleration Definition:
In circular motion, an acceleration acts on the body, whose direction is always towards the centre of the path. This acceleration is called centripetal acceleration.

Centripetal Acceleration Formula:
Centripetal acceleration, a = \(\frac{v^{2}}{r}\) = r ω²

Centripetal acceleration is also called radial acceleration as it acts along radius of circle.
Centripetal Acceleration Units:
Its unit is m/s² and it is a vector quantity.

Motion in a Plane (Projectile and Circular Motion):

Motion in a Plane Projectile Motion
Circular Motion Centripetal Acceleration
Centripetal and Centrifugal Force Examples of Centripetal Force in Everyday Life
Motion in Vertical Circle

Circular Motion | Definition, Equations, Formulas, Units – Motion in a Plane

Circular Motion Definition
Circular motion is the movement of an object in a circular path.

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Circular Motion | Definition, Equations, Formulas, Types, Units – Motion in a Plane

Circular Motion Types:
1. Uniform Circular Motion Definition:
If the magnitude of the velocity of the particle in circular motion remains constant, then it is called uniform circular motion.

2. Non-uniform Circular Motion Definition:
If the magnitude of the velocity of the body in circular motion is not constant, then it is called non-uniform circular motion.
Note:
Spinning Motion Definition:

A special kind of circular motion where an an object rotates around itself is called as spinning motion.

Variables in Circular Motion
(i) Angular Displacement Definition:
Angular displacement is the angle subtended by the position vector at the centre of the circular path.

Angular Displacement Formula
Angular displacement (Δθ) = \(\frac{\Delta s}{r}\)

where, As is the linear displacement and r is the radius.

Angular Displacement Units
SI unit is radian.

(ii) Angular Velocity Definition:
The time rate of change of angular displacement (Aθ) is called angular velocity.

Angular Velocity Formula
Angular velocity (ω) = \(\frac{\Delta \theta}{\Delta t}\)
Angular velocity is a vector quantity

Angular Velocity Units
SI unit is rad/s.

Relation between linear velocity (v) and angular velocity (ω) is given by
v = rω

(iii) Angular Acceleration Definition:
The rate of change of angular velocity is called angular acceleration.

Angular Acceleration Formula:
Angular acceleration (α) = \(\lim _{\Delta t \rightarrow 0} \frac{\Delta \omega}{\Delta t}=\frac{d \omega}{d t}=\frac{d^{2} \theta}{d t^{2}}\)

Angular Acceleration Units
SI unit is rad/s²

Angular Acceleration Dimensional Formula
dimensional formula is [T-2].

Relation between linear acceleration (α) and angular acceleration (α)
a =r α
where, r = radius.
Relation between angular acceleration and linear velocity
α = \(\frac{v^{2}}{r}\)

Non-uniform Horizontal Circular Motion
In non-uniform horizontal circular motion, the magnitude of the velocity of the body changes with time.
In this condition, centripetal (radial) acceleration (aR) acts towards centre and a tangential acceleration (aT) acts towards tangent.
Both acceleration acts perpendicular to each other.
Resultant acceleration, \(a=\sqrt{a_{R}^{2}+a_{T}^{2}}=\sqrt{\left(\frac{v^{2}}{r}\right)^{2}+(r \alpha)^{2}}\)
and

\(\tan \phi=\frac{a_{T}}{a_{R}}=\frac{r^{2} \alpha}{v^{2}}\)
where, α is the angular acceleration, r is the radius and v is the velocity.

Kinematic Equations in Circular Motion

Relations between different variables for an object executing circular motion are called kinematic equations in circular motion.
(i) ω = ω0 + αt
(ii) θ = ω0t + \(\frac{1}{2}\)αt²
(iii) ω² = ω0² + 2αθ
(iv) θt = ω0 + \(\frac{1}{2}\)α (2t -1)
(v) θ = \(\left(\frac{\omega+\omega_{0}}{2}\right)\)t
where, ω0 = initial angular velocity,
ω = final angular velocity,
α = angular acceleration,
θ = angular displacement,
θt = angular displacement at t seconds and t = time.

Motion in a Plane (Projectile and Circular Motion):
In this chapter or under this topic, we are going to come across the motion of the object when it is thrown from one end to another end. This practice is said to be projection. Also, when an object is moved in a circular motion, then the equation of the motion is derived here. We will learn here about centripetal force and centripetal acceleration in detail with formulas. Also learn the force applied in everyday life motion of the particle in a vertical circle.

Motion in a Plane Projectile Motion
Circular Motion Centripetal Acceleration
Centripetal and Centrifugal Force Examples of Centripetal Force in Everyday Life
Motion in Vertical Circle