A balloon and its content having mass M is moving up with an acceleration 'a'. The mass that must be released from the content so that the balloon starts moving up with an acceleration '3a' will be : (Take 'g' as acceleration due to gravity) [cite: 174, 175]
Substitute the value of F$F$ from Case 1 into Case 2 [cite: 836, 839]:
M(g + a) - (M - x)g = (M - x)3a$$M(g + a) - (M - x)g = (M - x)3a$$M g + M a - M g + x g = 3 M a - 3 x a$$M g + M a - M g + x g = 3 M a - 3 x a \quad \text{}$$M a + x g = 3 M a - 3 x a$$M a + x g = 3 M a - 3 x a$$x(g + 3a) = 2 M a$$x(g + 3a) = 2 M a$$x = (2 M a)/(3a + g)$$x = \frac{2 M a}{3a + g} \quad \text{}$$
Step 1: Visual Context
The free-body force layout for both accelerating phases is shown below:
Newton Second Law Applications free body diagrams for Q20
Newton Second Law Applications free body diagrams for Q20
Pattern Recognition
Since the upward buoyant force is completely determined by the balloon's volume, it remains constant. Expressing this constant force in terms of the initial conditions allows you to quickly solve for mass changes when acceleration states vary.
A ball of mass 0.5~kg$0.5\mathrm{~kg}$ is attached to a string of length 50~cm$50\mathrm{~cm}$. The ball is rotated on a horizontal circular path about its vertical axis. The maximum tension that the string can bear is 400~N$400\mathrm{~N}$. The maximum possible value of angular velocity of the ball in rad/s$\mathrm{rad/s}$ is:
A. 1600
B. 40
C. 1000
D. 20
Solution
Related Formula
Centripetal force configuration for simplified horizontal rotation layout:
T = mω² l$T = m\omega^2 l$
Core Logic
Given values:
m = 0.5~kg$m = 0.5\mathrm{~kg}$, l = 50~cm = 0.5~m$l = 50\mathrm{~cm} = 0.5\mathrm{~m}$, Tmax = 400~N$T_{\text{max}} = 400\mathrm{~N}$.
Ensure units are metric (50~cm → 0.5~m$50\mathrm{~cm} \to 0.5\mathrm{~m}$). Direct mapping to horizontal string projection metrics.
Chapter Mix
Class 11 Physics: Laws of Motion
Q36jee_main_2024_29_january_eveningCircular Motion and Tension
A stone of mass 900 g$900\text{ g}$ is tied to a string and moved in a vertical circle of radius 1 m$1\text{ m}$ making 10 rpm$10\text{ rpm}$. The tension in the string, when the stone is at the lowest point is (if π² = 9.8$\pi^2 = 9.8$ and g = 9.8 m/s²$g = 9.8\text{ m/s}^2$):
A.97 N$97\text{ N}$
B.9.8 N$9.8\text{ N}$
C.8.82 N$8.82\text{ N}$
D.17.8 N$17.8\text{ N}$
Solution
Related Formula
At the lowest point of a vertical circle, the equation of motion for a mass m$m$ is:
T - mg = m r ω²$$T - mg = m r \omega^2$$
Rearranging to solve for tension T$T$:
T = mg + m r ω²$$T = mg + m r \omega^2$$
Core Logic
Given data:
Mass, m = 900 g = 0.9 kg$m = 900\text{ g} = 0.9\text{ kg}$
Free-body diagram of stone at lowest point in vertical circle for Q36
Pattern Recognition
Always convert Mass to kg$\text{kg}$ and rotational speed to rad/s$\text{rad/s}$ first. Using the prompt constraint π² = 9.8$\pi^2 = 9.8$ yields a perfect decimal addition match.
A particle is moving in a circle of radius 50 cm$50\text{ cm}$ in such a way that at any instant the normal and tangential components of its acceleration are equal. If its speed at t = 0$t = 0$ is 4 m/s$4\text{ m/s}$, the time taken to complete the first revolution will be (1)/(α)[ 1 - e-2π ] s$\frac{1}{\alpha}\left[ 1 - e^{-2\pi} \right]\text{ s}$, where α =$\alpha =$ ________.
Numerical Answer.Answer: 8 to 8
Solution
Related Formula
For a particle in circular motion:
Normal (centripetal) acceleration: ac = (v²)/(r)$a_c = \frac{v^2}{r}$
Comparing this to (1)/(α)[ 1 - e-2π ] s$\frac{1}{\alpha}\left[ 1 - e^{-2\pi} \right]\text{ s}$, we get:
α = 8$\alpha = 8$
Pattern Recognition
The condition aₜ = ac v (dv)/(ds) = (v²)/(r) (dv)/(v) = (ds)/(r)$a_t = a_c \implies v \frac{dv}{ds} = \frac{v^2}{r} \implies \frac{dv}{v} = \frac{ds}{r}$. Integrating directly gives v = v₀ es/r$v = v_0 e^{s/r}$. Substituting this back into v = ds/dt$v = ds/dt$ makes the final time integral much more intuitive.
Chapter Mix
Class 11 Physics: Laws of Motion
Q36jee_main_2024_27_jan_morningBanking of Tracks
A train is moving with a speed of 12 m/s$12\text{ m/s}$ on rails which are 1.5 m$1.5\text{ m}$ apart. To negotiate a curve of radius 400 m$400\text{ m}$, the height by which the outer rail should be raised with respect to the inner rail is (Given, g = 10 m/s²$g = 10\text{ m/s}^{2}$):
A.6.0 cm$6.0\text{ cm}$
B.5.4 cm$5.4\text{ cm}$
C.4.8 cm$4.8\text{ cm}$
D.4.2 cm$4.2\text{ cm}$
Solution
Related Formula
θ = (v²)/(Rg)$$\tan\theta = \frac{v^2}{Rg}$$
For small angles, θ ≈ θ = (h)/(d)$\tan\theta \approx \sin\theta = \frac{h}{d}$, where h$h$ is the raised height and d$d$ is the separation between the tracks.
Whenever θ$\theta$ is small, geometry permits approximating θ$\tan\theta$ with hwidth$\frac{h}{\text{width}}$, vastly reducing computational transcendental overhead.
Chapter Mix
Class 11 Physics: Laws of Motion
Q45jee_main_2024_27_jan_morningConservation of Linear Momentum
A body of mass 1000 kg$1000\text{ kg}$ is moving horizontally with a velocity 6 m/s$6\text{ m/s}$. If 200 kg$200\text{ kg}$ extra mass is added, the final velocity (in m/s) is:
A.6$6$
B.2$2$
C.3$3$
D.5$5$
Solution
Related Formula
m₁ v₁ = m₂ v₂$$m_1 v_1 = m_2 v_2$$
Core Logic
Since there is no external horizontal force acting on the body, linear momentum along the horizontal axis is conserved.
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