Easy Projectile Motion Notes with Formulas for NEET Students
PROJECTILE MOTION
│
├── Definition
│ ├── Object thrown in air
│ ├── Moves under gravity only
│ └── Called projectile
│
├── Examples
│ ├── Cricket ball
│ ├── Football
│ ├── Stone
│ └── Bullet
│
├── Types of Motion
│ │
│ ├── Horizontal Motion
│ │ ├── Along x-axis
│ │ ├── No acceleration
│ │ ├── Constant velocity
│ │ └── Uniform motion
│ │
│ └── Vertical Motion
│ ├── Along y-axis
│ ├── Gravity acts downward
│ ├── Acceleration = g
│ └── Non-uniform motion
│
├── Galileo’s Concept
│ ├── Horizontal and vertical motions independent
│ └── Explained in 1632
│
├── Assumptions
│ ├── Air resistance neglected
│ └── Only gravity acts
│
├── Initial Velocity
│ ├── Total velocity = v₀
│ ├── Angle of projection = θ
│ │
│ ├── Horizontal Component
│ │ └── v₀x = v₀ cosθ
│ │
│ └── Vertical Component
│ └── v₀y = v₀ sinθ
│
├── Acceleration
│ ├── ax = 0
│ └── ay = -g
│
├── Position Equations
│ │
│ ├── Horizontal Position
│ │ └── x = (v₀ cosθ)t
│ │
│ └── Vertical Position
│ └── y = (v₀ sinθ)t - ½gt²
│
├── Velocity Equations
│ │
│ ├── Horizontal Velocity
│ │ └── vx = v₀ cosθ
│ │
│ └── Vertical Velocity
│ └── vy = v₀ sinθ - gt
│
├── Maximum Height
│ ├── Highest point
│ ├── vy = 0
│ └── Projectile changes direction
│
├── Trajectory
│ ├── Path followed by projectile
│ └── Shape = Parabola
│
├── Important NEET Points
│ ├── Horizontal velocity constant
│ ├── Gravity acts downward only
│ ├── vy = 0 at top point
│ ├── Path is parabolic
│ └── Motions are independent
│
└── Quick Tricks
├── cosθ → Horizontal
├── sinθ → Vertical
├── x-motion → Uniform
├── y-motion → Accelerated
└── Gravity acts vertically downward
![]() |
| Projectile motion showing horizontal and vertical components of motion with parabolic trajectory. |
Dr.Sanjaykumar pawar
Internal Links
Laws of Motion Notes for NEET
Motion in a Straight Line Notes
Motion in a Plane Complete Guide
Kinematics Formula Sheet
Gravitation Notes for NEET
Vectors Physics Notes
Work, Energy and Power Notes
Circular Motion NEET Notes
Physics Formula Revision Notes
NEET Physics Chapterwise Notes
Projectile Motion Notes for NEET Beginners
1. What is Projectile Motion?
A body thrown into the air and moving under the effect of gravity only is called a projectile.
The motion of such a body is called projectile motion.
Examples:
- Cricket ball
- Football
- Stone thrown in air
- Bullet fired at an angle
2. Main Idea of Projectile Motion
Projectile motion consists of two independent motions happening together.
(a) Horizontal Motion
- Motion along x-axis
- No acceleration acts horizontally
- Velocity remains constant
(b) Vertical Motion
- Motion along y-axis
- Gravity acts downward
- Acceleration is constant
3. Galileo’s Contribution
Galileo first explained that horizontal and vertical motions are independent of each other.
4. Assumption in Projectile Motion
- Air resistance is neglected.
- Only gravity acts on the projectile.
5. Initial Velocity of Projectile
Suppose a projectile is thrown with:
- Initial velocity = v0
- Angle of projection = θ
6. Components of Initial Velocity
(a) Horizontal Component
- Acts along x-axis
- Remains constant throughout motion
(b) Vertical Component
- Acts along y-axis
- Changes due to gravity
7. Acceleration of Projectile
- No horizontal acceleration
- Gravity acts vertically downward
8. Initial Position
This means the projectile starts from the origin.
9. Position of Projectile at Time t
(a) Horizontal Position
- Horizontal distance increases uniformly
- Depends on time and initial velocity
(b) Vertical Position
- Gravity slows upward motion
- Gravity increases downward motion
10. Velocity Components at Any Time
(a) Horizontal Velocity
Horizontal velocity remains constant.
(b) Vertical Velocity
Vertical velocity changes continuously because of gravity.
11. Maximum Height
At the highest point:
- Projectile stops moving upward for a moment
- Then it starts moving downward
12. Shape of Projectile Path
The path followed by a projectile is called a trajectory.
The trajectory of projectile motion is always a parabola.
13. Important NEET Points
- Horizontal velocity remains constant.
- Gravity acts only downward.
- Vertical velocity becomes zero at maximum height.
- Projectile path is parabolic.
- Horizontal and vertical motions are independent.
14. Formula Summary
Horizontal Velocity:
Vertical Velocity:
Horizontal Position:
Vertical Position:
15. Quick Revision Tricks
- cos θ → Horizontal component
- sin θ → Vertical component
- Horizontal motion → Constant velocity
- Vertical motion → Accelerated motion
- At highest point → vy = 0
16. Conclusion
Projectile motion is a combination of:
- Uniform horizontal motion
- Vertically accelerated motion under gravity
Projectile Motion Question Bank
Class 11 CBSE Physics
1. Multiple Choice Questions (MCQs)
b) Vertical velocity remains constant
c) Horizontal and vertical motions are independent
d) Gravity acts horizontally
b) g upward
c) g downward
d) Infinite
b) Minimum
c) Zero
d) Infinite
b) Decreases
c) Remains constant
d) Becomes zero
2. Very Short Answer Questions
3. Short Answer Questions
2. Only gravity acts on the projectile.
y = (v₀ sinθ)t − ½gt²
4. Long Answer Questions
- Horizontal Motion: No acceleration acts horizontally. Therefore horizontal velocity remains constant.
- Vertical Motion: Gravity acts vertically downward. Therefore vertical velocity changes continuously.
v₀x = v₀ cosθ
v₀y = v₀ sinθ
Position equations:
x = (v₀ cosθ)t
y = (v₀ sinθ)t − ½gt²
Velocity equations:
vx = v₀ cosθ
vy = v₀ sinθ − gt
The path followed by projectile is a parabola.
5. Assertion and Reason Questions
Reason (R): Gravity stops acting at maximum height.
Reason (R): No horizontal acceleration acts on projectile.
6. Fill in the Blanks
7. Case Study Questions
8. Statement Based Questions
9. Match the Columns
| Column A | Column B |
|---|---|
| 1. Horizontal acceleration | a. Parabola |
| 2. Path of projectile | b. Zero |
| 3. Vertical acceleration | c. g |
| 4. Highest point | d. vy = 0 |
1 → b
2 → a
3 → c
4 → d
10. HOTS Questions
11. Important Formulae
v₀y = v₀ sinθ
x = (v₀ cosθ)t
y = (v₀ sinθ)t − ½gt²
vx = v₀ cosθ
vy = v₀ sinθ − gt

Comments
Post a Comment