A small block of mass m slides down from the top of a frictionless inclined surface, while the inclined plane is moving towards left with constant acceleration a₀$a_{0}$ . The angle between the inclined plane and ground is θ$\theta$ and its base length is L. Assuming that initially the small block is at the top of the inclined plane, the time it takes to reach the lowest point of the inclined plane is ____.
A mass m on an inclined plane of base L, accelerating to the left with a0.
s = ut + (1)/(2)at²$$s = ut + \frac{1}{2}at^2$$Fpseudo = m a₀$$F_{\text{pseudo}} = m a_0$$
Core Logic
A mass m on an inclined plane of base L, accelerating to the left with a0.
We solve the problem from the non-inertial frame of reference of the inclined plane. A pseudo force m a₀$m a_0$ acts on the block towards the right.
Forces acting parallel to the incline (downward positive):
Component of gravity: mg θ$mg \sin \theta$
Component of pseudo force (pointing up the incline): -ma₀ θ$-ma_0 \cos \theta$
Step 1: Calculate Effective Acceleration
Net force down the incline:
Fₙₑₜ = mg θ - m a₀ θ$$F_{\text{net}} = mg \sin \theta - m a_0 \cos \theta$$
Thus, the acceleration relative to the incline is:
a = g θ - a₀ θ$$a = g \sin \theta - a_0 \cos \theta$$
Step 2: Distance Travelled
The base length of the incline is L$L$. Thus, the total length of the inclined surface is:
Whenever an inclined plane accelerates horizontally, resolve the pseudo force ma₀$ma_0$ parallel and perpendicular to the incline. Multiply by 2 inside the root to simplify into double-angle formats if options demand it.
Chapter Mix
Class 11 Physics: Laws of Motion
Class 11 Physics: Kinematics
Keywords:#slides down from the top of a frictionless inclined surface#JEE Main 2026 Evening Q40#Laws of Motion JEE Main 2026#Pseudo Force and Inclined Plane JEE Main 2026#Inclined plane#acceleration a0#mass m#angle theta#base length L
More Laws of Motion Previous-Year Questions — Page 6
Q39jee_main_2024_29_jan_morningFriction and Work Done
A block of mass 100 ~kg$100 \mathrm{~kg}$ slides over a distance of 10 ~m$10 \mathrm{~m}$ on a horizontal surface. If the co-efficient of friction between the surfaces is 0.4, then the work done against friction (in J) is:
A. 4200
B. 3900
C. 4000
D. 4500
Solution
Related Formula
Kinetic frictional force (f$f$) on a flat surface:
Wagainst = f · s = 400 ~N × 10 ~m = 4000 ~J$$W_{\text{against}} = f \cdot s = 400 \mathrm{~N} \times 10 \mathrm{~m} = 4000 \mathrm{~J}$$
Therefore, the work done is 4000 ~J$4000 \mathrm{~J}$.
Pattern Recognition
Work done by friction is negative (-4000 ~J$-4000 \mathrm{~J}$) because the frictional force opposes displacement. Work done against friction is positive (+4000 ~J$+4000 \mathrm{~J}$) because it represents the external energy that must be spent to sustain slide.
Chapter Mix
Class 11 Physics: Laws of Motion
Qjee_main_2024_30_january_eveningConnected Bodies and Tension
Three blocks A$\mathrm{A}$, B$\mathrm{B}$ and C$\mathrm{C}$ are pulled on a horizontal smooth surface by a force of 80N$80\mathrm{N}$ as shown in figure
Three masses (5 kg, 3 kg, 2 kg) connected by strings with tensions T1 and T2, being pulled by a common force F = 80N.
The tensions T₁$\mathrm{T}_{1}$ and T₂$\mathrm{T}_{2}$ in the string are respectively:
Tension at any point in a train of connected accelerating bodies (without friction) is directly proportional to the total mass being pulled behind that point.
Chapter Mix
Class 11 Physics: Laws of Motion
Q32jee_main_2024_30_january_eveningWork Done by Friction on Incline
A block of mass 1 ~kg$1 \mathrm{~kg}$ is pushed up a surface inclined to horizontal at an angle of 60°$60^{\circ}$ by a force of 10 ~N$10 \mathrm{~N}$ parallel to the inclined surface as shown in figure. When the block is pushed up by 10 ~m$10 \mathrm{~m}$ along inclined surface, the work done against frictional force is: [g = 10 ~m / s²]$\left[\mathrm{g} = 10 \mathrm{~m} / \mathrm{s}^{2}\right]$A block of mass M on an incline at 60 degrees, pulled by 10 N force, with coefficient of static friction 0.1.
A.5√(3) ~J$5\sqrt{3} \mathrm{~J}$
B.5 ~J$5 \mathrm{~J}$
C.5 × 10³ ~J$5 \times 10^{3} \mathrm{~J}$
D.10 ~J$10 \mathrm{~J}$
Solution
Related Formula
Wf = fk · d$$W_f = f_k \cdot d$$
fk = μ N$f_k = \mu N$
N = mg θ$$N = mg \cos\theta$$
Core Logic
The work done against the frictional force is the product of the kinetic friction force and the displacement along the plane.
The normal force N$N$ on the block is given by N = mg θ$N = mg \cos\theta$, where θ = 60°$\theta = 60^{\circ}$.
Whenever asked for "work done against friction", simply compute μ mg θ × d$\mu mg \cos\theta \times d$. The applied force (10 ~N$10 \mathrm{~N}$) is irrelevant to the friction calculation itself since it is parallel to the plane.
Chapter Mix
Class 11 Physics: Laws of Motion
Class 11 Physics: Work, Energy and Power
Q39jee_main_2024_30_january_eveningEquilibrium on a Rough Parabolic Curve
A block of mass m$m$ is placed on a surface having vertical cross section given by y = x² / 4$y = x^2 / 4$. If coefficient of friction is 0.5$0.5$, the maximum height above the ground at which block can be placed without slipping is:
For a block to remain stationary on a rough surface without slipping, the maximum slope of the surface it can rest on is determined by the angle of repose.
θ ≤ μ$$\tan \theta \le \mu$$
The slope of the given parabolic curve at any point (x,y)$(x,y)$ is dydx$\frac{\mathrm{d}y}{\mathrm{d}x}$.
When asked for maximum height on a curve y=f(x)$y=f(x)$ without slipping, set dydx = μ$\frac{\mathrm{d}y}{\mathrm{d}x} = \mu$, solve for x$x$, and plug it back into the original equation to find y$y$.
Chapter Mix
Class 11 Physics: Laws of Motion
Q32jee_main_2024_30_jan_morningConstraint Motion and Pulleys
All surfaces shown in figure are assumed to be frictionless and the pulleys and the string are light. The acceleration of the block of mass 2 ~kg$2 \mathrm{~kg}$ is:
Illustration of a 2kg block on a 30 degree incline attached via a pulley system to a 4kg hanging block.
A.g$g$
B.(g)/(3)$\frac{g}{3}$
C.(g)/(2)$\frac{g}{2}$
D.(g)/(4)$\frac{g}{4}$
Solution
Related Formula
Σ F = ma$$\sum F = ma$$a₁ = Constraint relation× a₂$$a_1 = \text{Constraint relation}\times a_2$$
Core Logic
Illustration of a 2kg block on a 30 degree incline attached via a pulley system to a 4kg hanging block.
Let the tension in the string attached to the 2 ~kg$2 \mathrm{~kg}$ block be T$T$. By tracing the string around the movable pulley, the tension supporting the 4 ~kg$4 \mathrm{~kg}$ mass becomes 2T$2T$.
From the principle of virtual work (or string constraints), if the 4 ~kg$4 \mathrm{~kg}$ block moves down with an acceleration a$a$, the string shortens by 2x$2x$ on the incline side, meaning the 2 ~kg$2 \mathrm{~kg}$ block moves up the incline with an acceleration of 2a$2a$.
Step 1: Write Equations of Motion
For the 4 ~kg$4 \mathrm{~kg}$ block (moving downwards):
4g - 2T = 4a$4g - 2T = 4a$
40 - 2T = 4a (i)$$40 - 2T = 4a \quad \dots (i)$$
For the 2 ~kg$2 \mathrm{~kg}$ block (moving up the incline):
Since g = 10 ~m/s²$g = 10 \mathrm{~m/s^2}$, this acceleration is exactly (g)/(3)$\frac{g}{3}$.
Pattern Recognition
Movable pulleys double the force but halve the displacement/acceleration on the supported side. Tension on the movable pulley side is twice the tension on the single string side. Remember to explicitly solve for the requested block's specific acceleration, not just 'a'.
Chapter Mix
Class 11 Physics: Laws of Motion
More Laws of Motion Questions — jee_main_2026_28_january_evening
Practice past-year questions one chapter at a time. Pick an exam → subject → chapter and get every PYQ for that topic — pulled together from all past papers — with the chapter's key formulas alongside.