A train consists of an engine and 3 coaches, first coach is closest to the engine, third coach is farthest from engine. The train is moving with a constant acceleration a. The mass of each coach is M. The force exerted by the first coach on the second coach will be:
Ma
2Ma
3Ma
4Ma
\(\sqrt{2}\)Ma
Given:
Step 1: Analyze Forces on Coach 2
For Coach 2 to accelerate at \( a \), the net force acting on it must be \( Ma \). This force is provided by:
Step 2: Consider Coach 3's Resistance
Coach 3 has mass \( M \) and must also accelerate at \( a \), requiring force \( Ma \). This force comes entirely from Coach 2 pushing it forward (\( F_{2 \rightarrow 3} = Ma \)).
By Newton's 3rd Law, Coach 3 exerts an equal and opposite force on Coach 2: \( F_{3 \rightarrow 2} = -Ma \).
Step 3: Apply Newton's 2nd Law to Coach 2
The net force on Coach 2 is:
\[ F_{1 \rightarrow 2} + F_{3 \rightarrow 2} = Ma \]
Substitute \( F_{3 \rightarrow 2} \):
\[ F_{1 \rightarrow 2} - Ma = Ma \]
\[ F_{1 \rightarrow 2} = 2Ma \]
Conclusion:
The force exerted by the first coach on the second coach is \( 2Ma \).
Answer: \(\boxed{B}\)
To determine the force exerted by the first coach on the second coach in a train moving with a constant acceleration \( a \), we can analyze the forces acting on each coach individually. Here is the step-by-step solution:
1. Understanding the setup:
- The train consists of an engine and 3 coaches.
- Each coach has mass \( M \).
- The train is accelerating with acceleration \( a \).
2. Analyzing forces on the third coach:
- The third coach is the farthest from the engine and only experiences the force exerted by the second coach.
- Let's denote the force exerted by the second coach on the third coach as \( F_{23} \).
- Using Newton's second law for the third coach:
\[ F_{23} = Ma \]
3. Analyzing forces on the second coach:
- The second coach experiences the force exerted by the first coach (denoted as \( F_{12} \)) and the reaction force from the third coach \( -F_{23} \).
- Using Newton's second law for the second coach:
\[ F_{12} - F_{23} = Ma \]
- Substituting \( F_{23} = Ma \) into the equation:
\[ F_{12} - Ma = Ma \]
\[ F_{12} = Ma + Ma \]
\[ F_{12} = 2Ma \]
Thus, the force exerted by the first coach on the second coach is \( 2Ma \).
So, The correct answer is Option (B): 2Ma
1. Visualize the system:
We have an engine pulling three coaches. The first coach is closest to the engine, and the third coach is farthest. The train is accelerating with a constant acceleration 'a'.
2. Consider the forces on the coaches:
The engine pulls all three coaches. The first coach pulls the second and third coaches. The second coach pulls the third coach.
3. Focus on the force exerted by the first coach on the second coach:
The first coach needs to accelerate its own mass and the mass of the two coaches behind it. The total mass being pulled by the first coach is 2M (the second and third coaches).
4. Apply Newton's second law:
Force (F) = mass (m) × acceleration (a)
In this case, the mass being accelerated by the force exerted by the first coach is 2M, and the acceleration is 'a'. Therefore:
\[F = (2M) \times a = 2Ma\]
y = a sin(βx + γt)wherex and t represent displacement and time, respectively. Then, the dimensional formula for β— γis:
If \( 2 \) is a solution of the inequality \( \frac{x-a}{a-2x}<-3 \), then \( a \) must lie in the interval:
A projectile is an object set in flight by applying an external force. The projectile may be thrown up vertically or at an angle to the horizontal. It may be dropped from a position of rest. The only force acting on the projectile during its motion along the flight path is the gravitational force and it is in motion due to its own inertia.
Examples of projectile are: a ball hit by a bat, bullet fired from a gun, shell launched from a launcher, bomb dropped from a plane, etc. It must be noted that a rocket or a missile cannot be considered as a projectile as they are propelled by power.
When a particle is thrown obliquely near the earth’s surface, it moves along a curved path under constant acceleration that is directed towards the centre of the earth (we assume that the particle remains close to the surface of the earth). The path of such a particle is called a projectile and the motion is called projectile motion or trajectory motion.
In a Projectile Motion, there are two simultaneous independent rectilinear motions:
Acceleration in the horizontal projectile motion and vertical projectile motion of a particle: When a particle is projected in the air with some speed, the only force acting on it during its time in the air is the acceleration due to gravity (g). This acceleration acts vertically downward. There is no acceleration in the horizontal direction, which means that the velocity of the particle in the horizontal direction remains constant.
The types of Projectile Motion Formula are: