Respondeu · bate com a resposta de referência dos cursinhos
a) \dfrac{V^2}{8g}(0{,}7)^{2n}; b) \dfrac{10V}{3g}.
levou 27 s
Como pensou
Seja e=0{,}7 o coeficiente de restituição. As componentes iniciais da velocidade são
v_{x,0}=V\cos30^\circ=\frac{\sqrt3V}{2},
\qquad
v_{y,0}=V\sen30^\circ=\frac V2.
Como o solo é perfeitamente liso, a componente horizontal permanece constante. Em cada choque, a componente vertical inverte o sentido e tem seu módulo multiplicado por e.
a) Altura máxima após n choques
Imediatamente após o n-ésimo choque, a velocidade vertical é
v_{y,n}=e^n\frac V2.
No ponto mais alto do voo seguinte, a velocidade vertical é nula. Assim,
0=v_{y,n}^2-2gh_n
\quad\Rightarrow\quad
\boxed{h_n=\frac{V^2}{8g}(0{,}7)^{2n}}.
b) Intervalo de tempo até a energia mínima
Adotando energia potencial nula no solo, a energia mecânica durante o voo após o n-ésimo choque vale
E_n=\frac12m v_x^2+\frac12m v_{y,n}^2
=\frac{3mV^2}{8}+\frac{mV^2}{8}e^{2n}.
Ela diminui a cada choque, tendendo ao mínimo
E_{\min}=\frac{3mV^2}{8},
correspondente ao movimento apenas horizontal.
O tempo de cada voo completo é
\Delta t_n=\frac{2v_{y,n}}g=\frac Vg e^n,
sendo n=0 o voo anterior ao primeiro choque. Portanto, o tempo total até cessar o movimento vertical é a soma geométrica
t=\sum_{n=0}^{\infty}\Delta t_n
=\frac Vg\frac1{1-e}
=\boxed{\frac{10V}{3g}}.
No modelo ideal, os infinitos choques acumulam-se nesse intervalo finito.
Resposta final: a) \dfrac{V^2}{8g}(0{,}7)^{2n}; b) \dfrac{10V}{3g}.
Respondeu · bate com a resposta de referência dos cursinhos
a) \dfrac{V^2}{8g}(0{,}7)^{2n}; b) \dfrac{10V}{3g}.
levou 18 s
Como pensou
Como o solo é perfeitamente liso, não há impulso horizontal nos choques. Portanto,
v_x=V\cos30^\circ=\frac{\sqrt3}{2}V
permanece constante. Já a componente vertical inicial é
v_{y0}=V\sin30^\circ=\frac V2.
a) Em cada choque, o módulo da velocidade vertical é multiplicado pelo coeficiente de restituição e=0{,}7. Como o projétil retorna ao solo com o mesmo módulo de velocidade vertical com que saiu, imediatamente após o n-ésimo choque temos
v_{y,n}=e^n\frac V2.
Assim, a altura máxima após esse choque é
h_n=\frac{v_{y,n}^2}{2g}
=\boxed{\frac{V^2}{8g}(0{,}7)^{2n}}.
b) Tomando a energia potencial gravitacional nula no solo, a energia mecânica após o n-ésimo choque é
E_n=\frac12m\left(v_x^2+v_{y,n}^2\right)
=\frac{3mV^2}{8}+\frac{mV^2}{8}(0{,}7)^{2n}.
Logo, a energia tende ao mínimo
E_{\min}=\frac{3mV^2}{8}
quando n\to\infty, isto é, quando cessa o movimento vertical.
O tempo de voo desde o lançamento até o primeiro choque é
\Delta t_0=\frac{2v_{y0}}g=\frac Vg.
Após o n-ésimo choque, o tempo até o choque seguinte é
\Delta t_n=\frac{2v_{y,n}}g=\frac Vg(0{,}7)^n.
Portanto, embora haja infinitos choques no modelo ideal, o tempo total é finito:
T=\sum_{n=0}^{\infty}\Delta t_n
=\frac Vg\frac{1}{1-0{,}7}
=\boxed{\frac{10V}{3g}}.
Resposta final: a) \dfrac{V^2}{8g}(0{,}7)^{2n}; b) \dfrac{10V}{3g}.
Respondeu · bate com a resposta de referência dos cursinhos
a) \displaystyle h_n=\frac{V^2}{8g}(0{,}49)^n; b) \displaystyle t=\frac{10V}{3g} (no limite de infinitos choques).
levou 30 s
Como pensou
**Analyzing energy in motion**
I'm considering the possibility that I'm interpreting the text "Quando necessário, use..." as an overall instruction. The launch angle doesn't need to be small; we're talking about 30 degrees. I think the problem has some nuances regarding the time intervals until the mass reaches the minimum of its energy, potentially after a series of collisions. I might need to rephrase the question about the time until the mass hits its energy minimum post-collisions. Horizontal kinetic energy remains constant since the plane is smooth.**Exploring time intervals and energy**
I'm thinking about whether the question regarding the "interval of time" could ask for the duration between two extrema. It might be better phrased as "para que ... atinja o mínimo da sua energia," meaning the time to reach the first energy minimum. I wonder if we're measuring mechanical energy from launch, which remains constant except for losses during collisions. The minimum energy over time is horizontal kinetic energy, approached asymptotically. They might expect that the interval for the mass to reach minimum energy is the sum of flight durations over infinite bounces, resembling a finite geometric series!**Analyzing energy dynamics**
I'm diving into the concept of flight time and energy behaviors. The mass stops bouncing at a limiting time, which relates to Zeno's paradox and the idea of minimum energy. The phrase about the time for mass to reach minimum energy probably refers to its kinetic energy. Even after infinite bounces, it suggests a finite collision time, where accumulated bouncing approaches energy minimum. This all depends on various factors like e, velocity, and angle, making part b quite intriguing!**Exploring kinetic energy and time**
I'm examining a smooth horizontal plane where horizontal velocity remains constant. The kinetic energy reaches its minimum when vertical velocity approaches zero, leading to a focus on horizontal kinetic energy. I wonder if this minimum can be obtained in finite time, given that there are infinitely many rebounds in that duration. The key is to consider the asymptotic and Zeno paradoxes. With calculations of flight durations and bounces, it ultimately wraps around to the time interval needed to reach minimum energy. There’s complexity here that’s fascinating!**Clarifying energy dynamics**
I'm looking at how total kinetic energy reaches its minimum at the apex, not when it hits the ground. The total mechanical energy, which includes both kinetic and potential energy, remains constant through segments but decreases after collisions. After each impact, the focused energy transitions to a horizontal kinetic state. I find it interesting that while energy values decrease with each collision, the limiting energy seems to be reached after bounces. I really need to explain this distinction between the different stages clearly!**Interpreting physical limits**
I'm working through a calculation about total elapsed time through impacts in physics, and I notice that as I sum through n impacts, I'm approaching a limit related to velocity and gravity. I realize there might be ambiguity depending on whether we're interpreting it in terms of mechanical energy or instantaneous kinetic energy. I could clarify both interpretations to make sure I address what was likely intended, especially regarding the time interval for the mass to reach minimum energy.**Considering collision mechanics**
I'm thinking about classic mechanics and how energy is lost with each collision, like an object bouncing on the floor. I’m curious about how long it takes for the object to stop bouncing completely. Since the coefficient of restitution (e) is less than 1, there will be infinitely many bounces, but the total time taken to stop bouncing can still be finite. It’s intriguing how this works within physical laws!**Evaluating minimum energy**
I think they want to know the total time to reach minimum energy, which might refer to the kinetic energy when at rest. Since this involves a perfectly smooth horizontal plane, the horizontal velocity is constant, meaning it never fully stops. This detail likely highlights that the minimum total kinetic energy is nonzero. If the plane were rough, there could be dissipation. They may also expect a time interval in Portuguese, asking for the time it takes to reach minimum energy. I'll clarify that this is a limiting sum and isn't attained at a finite time.**Exploring mechanical energy limits**
I think the total mechanical energy is minimal at the limit, and I could provide an energy formula for support. After the nth collision, the vertical energy ratio becomes e^(2n), approaching the base horizontal. I need to ensure I’m using mass properly and focus on velocities.
For durations, the initial flight time is t0 = V/g. After the j-th impact, the duration is t_j = e^j V/g, leading to a sum that converges; it shows the potential of infinitely many collisions occurring within finite time. The minimum energy is reached only as a limit, not at a finite time. At this limiting state, the vertical velocity becomes zero while the horizontal persists, giving Emin = 3mV²/8. Each trajectory's mechanical energy is constant, but it decreases at impacts.**Examining energy across trajectories**
At the apex, the mechanical energy remains constant during each flight, showing no variation across the sequence. The question about the "intervalo de tempo para que... atinja o mínimo da sua energia" could relate to the mass's minimum energy due to height. If we consider total energy, including potential energy, that makes sense. I’ll formulate a response in Portuguese, something like: "Como o plano não exerce impulso horizontal..." to tie it together nicely while addressing the minimum energy concept.
Seja e=0{,}7 o coeficiente de restituição. A componente horizontal da velocidade permanece constante, enquanto a componente vertical muda de sentido e tem seu módulo multiplicado por e a cada choque.
a) Imediatamente após n choques, a componente vertical da velocidade é
v_{y,n}=e^n V\sin 30^\circ=\frac{e^nV}{2}.
A altura máxima correspondente é
h_n=\frac{v_{y,n}^2}{2g}
=\frac{V^2}{8g}(0{,}7)^{2n}
=\frac{V^2}{8g}(0{,}49)^n.
b) O tempo de voo inicial, até o primeiro choque, é
\Delta t_0=\frac{2V\sin30^\circ}{g}=\frac Vg.
Após o k-ésimo choque, o tempo até o choque seguinte é
\Delta t_k=\frac{2e^kV\sin30^\circ}{g}=\frac{e^kV}{g}.
Assim, o tempo total até o limite dos choques é
t=\sum_{k=0}^{\infty}\Delta t_k
=\frac Vg\sum_{k=0}^{\infty}(0{,}7)^k
=\frac{10V}{3g}.
Nesse limite, a componente vertical da velocidade tende a zero. A energia mínima é, portanto, o limite da energia mecânica, que inclui a energia cinética horizontal, constante:
E_{\min}=\frac12m(V\cos30^\circ)^2=\frac{3mV^2}{8}.
Esse mínimo é atingido apenas no limite de infinitos choques; estes se acumulam em um tempo finito.
Resposta final: a) \displaystyle h_n=\frac{V^2}{8g}(0{,}49)^n; b) \displaystyle t=\frac{10V}{3g} (no limite de infinitos choques).
Respondeu · bate com a resposta de referência dos cursinhos
a) H_n = V²(0,7)^{2n}/(8g) = V²(0,49)ⁿ/(8g); b) Δt = 10V/(3g)
levou 15 s
Como pensou
Since the horizontal surface is frictionless, only the vertical velocity component shrinks with each bounce by the restitution factor e. Starting with vertical speed V/2, after n bounces it becomes (V/2)e^n, so I'm computing the maximum height from that reduced vertical velocity using the standard projectile height formula.
For part b, since energy keeps decreasing with each bounce but theoretically approaches a minimum only as n→∞, the total time is the sum of an infinite geometric series of flight times, each shrinking by factor e. With initial flight time V/g and ratio e=0,7, I'm summing the series to get total time = (V/g)/(1-e) = 10V/(3g).
Dados: V₀ₓ = V cos30° = V√3/2 (conserva-se, pois o solo é liso); V₀ᵧ = V sen30° = V/2; e = 0,7.
a) Altura máxima após n choques
A cada choque com o solo, apenas a componente vertical da velocidade é alterada:
v_y' = e·v_y.
Após n choques: v_y,n = (V/2)·eⁿ.
Altura máxima correspondente:
H_n = v_y,n²/(2g) = (V²/4)·e^{2n}/(2g) = V²·(0,7)^{2n}/(8g) = V²(0,49)ⁿ/(8g).
b) Tempo para atingir a energia mínima
A energia mínima é atingida quando a componente vertical da velocidade se anula (restando apenas a energia cinética horizontal, E_min = ½m(V√3/2)² = 3mV²/8), o que ocorre após infinitos choques, num tempo total finito.
Tempo do primeiro voo: T₀ = 2v_y/g = 2(V/2)/g = V/g.
Após o k-ésimo choque, o tempo de voo é T_k = (V/g)·eᵏ.
Tempo total (série geométrica):
T = (V/g)(1 + e + e² + ...) = (V/g)·1/(1 − e) = (V/g)·1/0,3 = 10V/(3g).
Resposta final: a) H_n = V²(0,7)^{2n}/(8g) = V²(0,49)ⁿ/(8g); b) Δt = 10V/(3g)
Respondeu · bate com a resposta de referência dos cursinhos
a) H_n = \dfrac{(0{,}49)^n V^2}{8g}; b) \Delta t = \dfrac{10V}{3g}
levou 15 s
Como pensou
I'm working out the vertical velocity decay with each bounce, giving max height after n bounces as (0.49)^n times V²/(8g), then starting to sum the total flight time across infinite bounces using the geometric series of successive airtimes.
Since mechanical energy only drops at impacts, not during flight, the minimum energy state occurs in the limit as the vertical motion dies out—so the total time to reach that minimum works out to 10V/(3g).
Decomposição da velocidade inicial
- Componente horizontal: V_x = V\cos 30^\circ = \dfrac{V\sqrt3}{2}.
- Componente vertical: V_y = V\sin 30^\circ = \dfrac{V}{2}.
Como o solo é perfeitamente liso, não há atrito. Nas colisões não há impulso horizontal, logo V_x permanece constante. O coeficiente de restituição atua só sobre a componente normal, que é a vertical: a cada choque, v_y \to e\,v_y, com e = 0{,}7.
a) Altura máxima após n choques
Após n choques, a componente vertical vale
v_{y,n} = e^n\frac{V}{2} = (0{,}7)^n\frac{V}{2}.
A altura máxima vem de v_{y,n}^2 = 2gH_n:
H_n = \frac{v_{y,n}^2}{2g} = \frac{(0{,}49)^n V^2}{8g}.
b) Tempo até a energia mínima
Durante cada voo a energia mecânica se conserva. Ela só diminui nos choques, que reduzem a parte vertical do movimento. A energia mínima é E_{min} = \tfrac12 m V_x^2 = \tfrac{3}{8}mV^2. Ela corresponde a v_y = 0, quando a massa passa a deslizar sobre o solo. Isso ocorre após infinitos choques, mas em tempo finito.
O tempo de cada voo é:
- 1º voo: t_0 = \dfrac{2(V/2)}{g} = \dfrac{V}{g}.
- Voo após o k-ésimo choque: t_k = \dfrac{V}{g}(0{,}7)^k.
O tempo total é a soma de uma progressão geométrica de razão 0,7:
T = \frac{V}{g}\sum_{k=0}^{\infty}(0{,}7)^k = \frac{V}{g}\cdot\frac{1}{1-0{,}7} = \frac{10V}{3g}.
Resposta final: a) H_n = \dfrac{(0{,}49)^n V^2}{8g}; b) \Delta t = \dfrac{10V}{3g}
Respondeu · bate com a resposta de referência dos cursinhos
a) H_n = (0,7)^{2n} V²/(8g) = (0,49)ⁿ V²/(8g); b) Δt = V/[g(1−e)] = 10V/(3g)
levou 14 s
Como pensou
I'm working out a projectile bouncing problem with horizontal launch at 30° and restitution coefficient e=0.7 affecting only vertical velocity. For part a), I derive the max height after n bounces as a function decaying with e^(2n); for part b), I'm considering how horizontal kinetic energy stays constant while vertical energy decays, to find the minimum energy condition.
Since vy approaches zero only after infinite bounces, the mass reaches minimum energy (purely horizontal) only in the limit, with total flight time being a geometric series summing to V/(g(1-e)) = 10V/(3g).
Hipóteses: o solo é perfeitamente liso, então não há atrito e a componente horizontal da velocidade se conserva: v_x = V cos 30°. Em cada choque, a componente vertical é multiplicada por e = 0,7 (inverte o sentido e perde módulo).
Velocidade vertical inicial: v_y0 = V sen 30° = V/2.
a) Altura máxima após n choques
Depois de n choques, a componente vertical vale v_yn = eⁿ·V/2. A altura máxima do salto seguinte é
H_n = v_yn² / (2g) = e²ⁿ V² / (8g)
H_n = (0,49)ⁿ · V²/(8g)
Para n = 0 recupera-se H₀ = V²/(8g), que é a altura do lançamento inicial.
b) Tempo para a energia mínima
A energia mecânica é a soma da energia cinética horizontal (constante, igual a ⅜mV²) com a parte associada ao movimento vertical (cinética e potencial). Essa segunda parte diminui a cada choque. A energia total é mínima quando o movimento vertical cessa, e a partir daí a massa apenas desliza sobre o solo, com E_min = ⅜mV².
O tempo de cada voo é proporcional a v_y:
- 1º voo (da origem até o 1º choque): t₀ = 2(V/2)/g = V/g
- voo após n choques: tₙ = eⁿ V/g
Embora haja infinitos choques, a soma dos tempos converge (série geométrica):
Δt = (V/g)(1 + e + e² + …) = V / [g(1 − e)] = V / (0,3 g)
Δt = 10V/(3g) ≈ 3,3 V/g
Resposta final: a) H_n = (0,7)^{2n} V²/(8g) = (0,49)ⁿ V²/(8g); b) Δt = V/[g(1−e)] = 10V/(3g)
Respondeu · bate com a resposta de referência dos cursinhos
a) \dfrac{(0{,}7)^{2n}V^{2}}{8g}; b) \dfrac{10V}{3g}
levou 1 min 12 s
Como pensou
The problem concerns projectile motion with restitution in Portuguese.
The problem involves an oblique launch from the origin with initial velocity at 30° to a perfectly smooth horizontal ground. The coefficient of restitution is 0.7. The task is to find the maximum height after n collisions and the time to reach minimum energy. Horizontal velocity remains constant. Vertical velocity changes by the factor e on each collision.
The initial vertical velocity is V/2 and the horizontal component is V√3/2. The first maximum height is V²/(8g). After each collision the vertical speed becomes e times its previous value, so the next peak height is (eV/2)²/(2g).
The maximum height after n collisions is h_n = (0.49)^n V²/(8g). The small-angle approximation hint was not used yet.
Energy is conserved between collisions but drops at each bounce. The minimum energy occurs after the last collision. The time interval to reach that minimum is the sum of all flight times between bounces.
The total time is finite because the flight durations form a convergent geometric series. After the final bounce, the mass slides horizontally with constant velocity and energy remains at its minimum value.
The first flight time is T0 = 2V/g. After each collision the upward speed becomes e times its previous value, so the next flight time is T1 = 2eV/g, then T2 = 2e²V/g, and so on. The total time to reach minimum energy is the sum of this geometric series over all bounces.
The total time to reach minimum energy is τ = V/(0.3g), or 10V/(3g). This is the sum of all flight times, since the geometric series converges to (2Vy/g)/(1−e) and Vy = V/2.
A componente horizontal da velocidade permanece constante, pois o solo é liso:
v_x=V\cos 30^\circ=\frac{V\sqrt{3}}{2}.
A componente vertical inicial é
v_y=V\sin 30^\circ=\frac{V}{2}.
O coeficiente de restituição atua somente sobre a componente vertical. Assim, imediatamente após o n-ésimo choque a velocidade vertical de subida vale e^n v_y, com e=0,7.
a) A altura máxima atingida nesse trecho é
H_n=\frac{(e^n v_y)^2}{2g}=\frac{(0,7)^{2n}V^2}{8g}.
b) O tempo de voo até o primeiro choque é V/g. Os tempos de voo subsequentes formam a progressão geométrica de razão e. A energia mecânica decresce apenas nos choques e atinge seu valor mínimo (apenas a energia cinética horizontal) quando os saltos cessam. O instante correspondente é a soma da série:
T=\frac{V/g}{1-0,7}=\frac{10V}{3g}.
Resposta final: a) \dfrac{(0{,}7)^{2n}V^{2}}{8g}; b) \dfrac{10V}{3g}
Respondeu · bate com a resposta de referência dos cursinhos
a) h_n=\dfrac{(0{,}49)^nV^2}{8g}; b) T=\dfrac{10V}{3g}
levou 39 s
Como pensou
We need answer in Portuguese, solve physics problem. Need parse images. Text: "Quando necessário, use a seguinte informação: Para θ << 1 assuma senθ ≈ θ." Then problem: "Considere um lançamento oblíquo de uma massa m, partindo da origem do plano xy, em que a velocidade inicial V faz um ângulo de 30° com a horizontal perfeitamente lisa. Sabendo que o coeficiente de restituição entre a massa m e o solo é 0,7, determine
a) a altura máxima após n choques;
b) o intervalo de tempo para que a massa m atinja o mínimo da sua energia."
We need solve. Let's think carefully.
Projectile launched from origin (x=0,y=0?) with initial speed V at angle 30° to horizontal. Ground is horizontal? "plano xy" origin, solo? "entre a massa m e o solo" implies ground at y=0? Velocity angle with horizontal. It lands and bounces. Coefficient of restitution e = 0.7 = 7/10. Need after n bounces max height? Need time interval for mass to reach minimum energy? Hmm.
"perfeitamente lisa" horizontal? "solo" maybe plane xy? The ground is x-axis? Let's parse: "partindo da origem do plano xy, em que a velocidade inicial V faz um ângulo de 30° com a horizontal perfeitamente lisa." Maybe "horizontal perfeitamente lisa" means ground is smooth horizontal plane? Launch from origin of xy plane; initial velocity V makes angle 30° with horizontal smooth surface. Coefficient of restitution between mass and ground 0.7. Determine:
a) maximum height after n collisions;
b) time interval for mass m to reach minimum energy.
We need derive.
Projectile launched from ground with speed V at angle 30. It travels parabolic path, strikes ground with vertical velocity component -V sin30 = -V/2? Actually initial vertical component V_y0 = V sin30 = V/2 upward; horizontal V_x = V cos30 = (√3/2)V, constant due no horizontal force (ground smooth). At impact, vertical component just before = -V sin30 (same magnitude downward) and horizontal same V cos30. Coefficient of restitution e = 0.7 applies to normal component: vertical component after bounce = e * vertical speed before? Usually restitution e = separation speed / approach speed along normal, so vertical rebound speed = e * initial vertical speed (magnitude) = e V/2. Horizontal component unchanged. After each bounce, vertical component reduced by factor e, horizontal unchanged. Time between bounces? After bounce, vertical component v_y = e^n? Let's define n collisions after initial launch. Before first collision, vertical speed magnitude V sin30. After first collision (n=1? "após n choques" means after n bounces), vertical component = e V sin30. Maximum height after n bounces occurs after leaving ground following nth collision, when vertical velocity becomes zero at apex. Height h_n = (v_y,n)^2 / (2g) = (e^n V sin30)^2/(2g)? Wait for n=0 (before any collision) initial height max = (V sin30)^2/(2g). After n choques, vertical speed after nth bounce is e^n V sin30 (assuming after nth collision). Then max height after n collisions = (e^n V sin30)^2/(2g) = e^{2n} V^2 sin^2 30 / (2g) = (e^{2n} V^2)/(8g) since sin30=1/2 -> sin^2=1/4 -> V^2/4 /2g = V^2/(8g). So h_n = e^{2n} V^2/(8g). Or maybe if n collisions means after n-th collision? Yes.
But question "altura máxima após n choques" maybe height after n bounces? Yes.
Part b: "o intervalo de tempo para que a massa m atinja o mínimo da sua energia." Minimum energy? Energy decreases due inelastic collisions. It will bounce infinitely many times, but total time? "intervalo de tempo para que a massa m atinja o mínimo da sua energia" maybe "time interval until it reaches minimum energy" = when it stops bouncing / energy minimum? But with coefficient of restitution 0.7, it never stops in finite time? Actually vertical motion after infinite bounces total time is finite? Let's see: time between bounces after initial? The total time from launch to rest for bouncing ball with restitution e < 1 is finite: t_total = ? Projectile vertical component. After each bounce, vertical speed reduces by factor e; flight time for each jump reduces by factor e. Total time = initial time to first bounce + sum_{k=1}∞ 2 * (v_y after kth bounce)/g? Actually Let's derive. Initial flight from launch to first impact: time t0 = 2 V sinθ / g? Because initial and landing at same height (origin y=0) due symmetry, time of flight = 2 V sinθ / g. After first bounce, vertical speed u1 = e V sinθ, flight time to next bounce (same level) t1 = 2 u1 / g = 2 e V sinθ / g. After second t2 = 2 e^2 V sinθ / g, etc. Total time until "rest" (infinite bounces) T = t0 + t1 + t2 + ... = (2 V sinθ/g)(1 + e + e^2 + ...) = (2 V sinθ/g)/(1 - e) = (2 V *1/2 / g)/(1 - e) = (V/g)/(1 - e) = V/[g(1-e)]. Since e=0.7, T = V/(0.3 g) = (10/3) V/g? Wait 0.3=3/10, reciprocal 10/3. So T = 10V/(3g). Is this "intervalo de tempo para que a massa m atinja o mínimo da sua energia"? It reaches minimum energy asymptotically as time tends to T? Actually energy minimum is when vertical kinetic energy zero and potential? At ground? Energy total includes kinetic + potential; at each bounce after infinite bounces, vertical kinetic energy tends zero, horizontal kinetic energy remains? Wait horizontal velocity constant V cos30 = √3 V/2, so kinetic energy horizontal remains (1/2)m (3/4 V^2) = 3mV^2/8. Potential energy at ground zero. Total energy tends horizontal kinetic energy = 3mV^2/8. It never reaches minimum? Actually as t approaches total time, height and vertical speed go to zero; horizontal speed remains. So energy minimum attained at t = T? At t=T? The particle would be at ground with vertical speed zero, horizontal speed V cosθ, so total energy = (1/2)m (V cosθ)^2 = (1/2)m V^2 * 3/4 = 3mV^2/8. Is there any subsequent? At t=T it stops bouncing (vertical motion stops) and continues sliding horizontally? Actually after infinite bounces, it slides along the ground with constant horizontal speed V cosθ, no further vertical motion. Energy minimum reached at T (limit). So answer interval maybe T = V/[g(1-e)]? But question asks "o intervalo de tempo para que a massa m atinja o mínimo da sua energia." Could mean "time interval" maybe from launch until it reaches minimum energy; yes total time to stop bouncing. So b) T = V/[g(1 - 0.7)] = V/(0.3g) = 10V/(3g). Need include maybe after infinite collisions? But finite. Let's check.
However, there is a subtlety: "o intervalo de tempo para que a massa m atinja o mínimo da sua energia" maybe "interval between bounces" when it reaches minimum energy? Actually "intervalo de tempo" could mean "time interval" between successive collisions? But phrase: "o intervalo de tempo para que a massa m atinja o mínimo da sua energia." Maybe it asks "the time interval for mass m to reach the minimum of its energy" (i.e., from launch until minimum energy). The word "intervalo" maybe duration. Yes.
But need consider horizontal motion and energy: horizontal component remains constant; vertical energy dissipates. Minimum energy when vertical motion ceases; total energy = horizontal kinetic energy = 1/2 m (V cos30)^2 = 3mV^2/8. Is this "mínimo da sua energia"? Potentially yes.
But could there be another interpretation: energy of mass includes gravitational potential? Minimum energy occurs at lowest height (ground). It reaches minimum energy at each bounce? At every contact with ground, potential energy zero; but immediately after bounce it has vertical kinetic energy so total energy > horizontal kinetic. As time goes on, at bounces the total energy decreases, approaching horizontal kinetic energy. "atinja o mínimo da sua energia" maybe exactly when it stops bouncing. So T total.
Let's ensure formulas match.
Now, need write solution as candidate in Portuguese, step-by-step.
Need mention coefficient of restitution e=0.7=7/10. Use g for gravity, maybe assume vertical acceleration g. Horizontal component unaffected. Let v0 = V. Decompose:
V_x = V cos30 = (√3/2)V.
V_y0 = V sen30 = V/2.
At each collision, vertical velocity after collision = e times vertical velocity before. Since gravitational acceleration constant, flight time and max height scale by e. After n collisions, vertical speed after nth collision is e^n V_y0 = e^n V/2. Then maximum height after n collisions:
h_n = (e^n V/2)^2 / (2g) = e^{2n} V^2/(8g). Wait compute: (e^n V/2)^2 = e^{2n} V^2/4; divide by 2g = e^{2n} V^2/(8g). Yes.
Alternatively, if they mean after n-th collision, n≥0? "após n choques" likely n choques = n bounces, n=1,2,... For n=0? Usually after n collisions means after n-th collision; if n=0 would be initial max height, not after any collision. We'll state para n choques (n ≥ 0? No, after n choques means after n bounces; n ≥ 1; if n=0, initial). But formula also works for n=0? It gives initial max height V^2/(8g). They might accept.
Part b: Time between consecutive impacts? For vertical motion, time between impacts after nth bounce: 2 v_y,n/g. Initial flight time (before first impact) t0 = 2 V_y0/g = V/g? Wait V_y0 = V/2, so t0 = 2*(V/2)/g = V/g. After first bounce, t1 = 2*(e V/2)/g = e V/g. After second, t2 = 2*(e^2 V/2)/g = e^2 V/g, etc. Total time until vertical motion ceases: T = t0 + t1 + ... = (V/g)(1 + e + e^2 + ...) = (V/g)/(1-e) = V/[g(1-e)] = V/(0.3g) = 10V/(3g). Actually check initial t0 = V/g yes. If someone might compute first impact time = V/g because V_y0 = V/2 => t_up = V/(2g), total V/g. Good.
At this limit, energy minimum = kinetic energy horizontal = 1/2 m V^2 cos^2 30 = 3mV^2/8, but question only asks interval? "o intervalo de tempo para que a massa m atinja o mínimo da sua energia." Could also ask "o intervalo de tempo" maybe time interval between successive collisions after it reaches minimum? No, minimum energy at infinite time, so interval? Hmm "o intervalo de tempo para que a massa m atinja o mínimo da sua energia" "the time interval for the mass m to reach the minimum of its energy." We'll answer T.
But let's be thorough: Could "mínimo da sua energia" refer to mechanical energy minimum at the moment of highest point of each bounce? No, highest potential energy? Actually "mínimo da energia" in projectile with drag? Inelastic bounces: after each bounce kinetic energy reduces; mechanical energy (kinetic + potential) changes during flight but at ground potential zero; total energy after bounce is less. Minimum energy occurs as n→∞. Yes.
Need possibly consider "horizontal perfeitamente lisa" and "coeficiente de restituição entre a massa m e o solo" could mean ground at y=0. The phrase "partindo da origem do plano xy" maybe origin at ground? "lançamento oblíquo ... partindo da origem do plano xy" likely origin at ground level. "plano xy" horizontal? The horizontal ground is the x-axis? OK.
Potential issue: The coefficient of restitution sometimes defined as ratio of speeds after and before in direction normal to plane; for ground, vertical component. Yes.
Need produce final answer with item labels. Could include "considere g a aceleração da gravidade." Need maybe mention "desprezando resistência do ar". The problem doesn't explicitly say no air resistance, but standard. "horizontal perfeitamente lisa" could mean no friction with ground; air resistance likely negligible.
Let's formulate in Portuguese:
Seja \(v_0=V\), \(e=0,7\). Componentes:
\(v_{0x}=V\cos30^\circ = \frac{\sqrt3}{2}V\) (constante)
\(v_{0y}=V\operatorname{sen}30^\circ = V/2\).
Após cada choque, a componente vertical fica multiplicada por e; a horizontal não muda. Assim, após n choques:
\(v_{y,n}=e^n V/2\).
A altura máxima após o n-ésimo choque:
\(h_n = \frac{v_{y,n}^2}{2g} = \frac{e^{2n}V^2}{8g}\).
b) Tempo entre dois choques consecutivos? Actually from launch to nth? We need total time. Let's derive:
O tempo de voo após o k-ésimo choque é \(\Delta t_k = 2 v_{y,k}/g = \frac{e^k V}{g}\)? Wait for k? Let's index carefully:
Before any choque (initial launch), time to first collision:
\(\Delta t_0 = \frac{2 v_{0y}}{g} = \frac{V}{g}\).
Após o primeiro choque, vertical speed \(e V/2\); time until next collision:
\(\Delta t_1 = \frac{2 (e V/2)}{g} = \frac{e V}{g}\).
Após o segundo choque: \(\Delta t_2 = e^2 V/g\), etc.
Total:
\(T = \sum_{k=0}^{\infty} \Delta t_k = \frac{V}{g}(1+e+e^2+\cdots) = \frac{V}{g(1-e)} = \frac{V}{0,3g} = \frac{10V}{3g}\).
No limite, a energia mecânica se reduz à energia cinética horizontal, \(E_{\min} = \frac12 m (V\cos30^\circ)^2 = \frac{3}{8}mV^2\), mas o item pede o intervalo de tempo.
Wait part b asks "o intervalo de tempo para que a massa m atinja o mínimo da sua energia." Maybe "intervalo de tempo" might be "time interval" maybe "tempo total" okay.
Let's check if there is any alternative: Some might solve for time until minimum energy by setting derivative of energy zero? But energy monotonically decreasing in vertical component; minimum at t=T. Good.
Potential challenge: "após n choques" maybe after n bounces, there is a maximum height. But for n=0, first max height; after first choque, max height after first bounce = e^2 V^2/(8g). But they may denote n choques = after n-th collision, n≥1. If n=0 ambiguous. We can note n≥0, fórmula geral.
Now consider if ground is "perfeitamente lisa" (frictionless) and coefficient of restitution "entre a massa m e o solo é 0,7" — for oblique bounce on a smooth horizontal plane, the normal impulse changes vertical component; tangential component unchanged because no friction. Correct.
Now "mínimo da sua energia" maybe could be "minimum of its energy" at the instant just before it stops bouncing, but because horizontal velocity remains, the mechanical energy after infinite bounces is \(\frac{3}{8}mV^2\). Could ask "intervalo de tempo" maybe between the first launch and the instant it reaches minimum energy. Yes.
Need perhaps mention "massa m" cancels in gravitational acceleration; no need mass.
Let's construct final response with equations and final answer.
Need include "Quando necessário..." assumption? Not needed, θ=30° not small. Or maybe use \(g\) not given. We should use \(g\).
Let's write final:
"Decompondo a velocidade inicial..."
\(V_{0x}=V\cos30^\circ\), \(V_{0y}=V\mathrm{sen}30^\circ=V/2\).
a) Após n choques:
\(V_{y,n}=e^n V_{0y}=e^n V/2\). A altura máxima é:
\(H_n = V_{y,n}^2/(2g) = (e^n V/2)^2/(2g)= e^{2n}V^2/(8g)\).
b) Tempo de voo inicial:
\(t_0=2V_{0y}/g = V/g\).
Tempo de voo após o k-ésimo choque? Need careful: after first collision, vertical component \(e V/2\), so time between first and second impact \(t_1=2(eV/2)/g = eV/g\). After n-th? Let's define \(t_k = e^k V/g\), k=0,1,2,... Actually t_0 corresponds before first impact; t_1 after first before second; t_n after n-th before (n+1)-th. Total:
\(T = \sum_{k=0}^\infty t_k = \frac Vg(1+e+e^2+\cdots)=\frac Vg\frac1{1-e}=\frac{V}{g(1-0,7)}=\frac{10V}{3g}\).
At this limit, \(E=E_{\min}\).
Then final answer: a) \(h_n= \dfrac{e^{2n}V^2}{8g} = \dfrac{(0,7)^{2n}V^2}{8g}\) (ou \(\dfrac{V^2}{8g}(0,49)^n\)); b) \(T=\dfrac{10V}{3g}\) (ou \(\dfrac{V}{0,3g}\)).
Need ensure coefficients: 0.7^{2n} = (0.49)^n. Yes. Since e=0.7, e^2=0.49.
Let's double-check formulas with n=1: h_1 = e^2 V^2/(8g) = 0.49 V^2/(8g) = 0.06125 V^2/g. Initial h_0 = V^2/(8g). After one bounce, max height 0.49 of initial. Good.
Part b T = V/(g(1-0.7)) = V/(0.3g) = 3.333 V/g. Initially t0 = V/g. Sum = V/g * (1/(0.3)) = 3.333 V/g. Good.
Potential issue: In part b, "intervalo de tempo para que a massa m atinja o mínimo da sua energia." Could also be "time interval between the instant it reaches minimum energy and something else"? No. It asks "o intervalo de tempo para que ... atinja ..." = duration until it reaches. Fine.
Need final line: "Resposta final: a) ...; b) ...". Could include units? No numeric values except V,g; okay.
Let's produce final in Portuguese with moderate detail.
Seja e=0{,}7=\dfrac{7}{10}. Decompomos a velocidade inicial:
V_x=V\cos30^\circ=\frac{\sqrt3}{2}V \quad\text{(constante)}
V_{y0}=V\operatorname{sen}30^\circ=\frac V2
Após cada choque, a componente vertical fica multiplicada por e, enquanto a horizontal permanece constante.
a) Após n choques, a componente vertical é
V_{y,n}=e^nV_{y0}=e^n\frac V2
Logo, a altura máxima após n choques é
h_n=\frac{V_{y,n}^2}{2g}
=\frac{\left(e^n\frac V2\right)^2}{2g}
=\frac{e^{2n}V^2}{8g}
Portanto,
h_n=\frac{(0{,}7)^{2n}V^2}{8g}
=\frac{(0{,}49)^nV^2}{8g}
b) O tempo de voo inicial é
t_0=\frac{2V_{y0}}{g}=\frac{2\cdot V/2}{g}=\frac Vg
Após o primeiro choque, a componente vertical é eV/2, então o tempo entre o primeiro e o segundo choque é
t_1=\frac{2(eV/2)}{g}=\frac{eV}{g}
Analogamente, o intervalo entre o k-ésimo e o (k+1)-ésimo choque é
t_k=\frac{e^kV}{g}
O tempo total até a massa atingir o mínimo de energia, isto é, até cessar o movimento vertical, é
T=\sum_{k=0}^{\infty}t_k
=\frac Vg(1+e+e^2+\cdots)
=\frac Vg\cdot\frac1{1-e}
Substituindo e=0{,}7:
T=\frac Vg\cdot\frac1{1-0{,}7}
=\frac Vg\cdot\frac1{0{,}3}
=\frac{10V}{3g}
Resposta final: a) h_n=\dfrac{(0{,}49)^nV^2}{8g}; b) T=\dfrac{10V}{3g}
Respondeu · bate com a resposta de referência dos cursinhos
a) \frac{V^2}{8g}(0,49)^n; b) \frac{10V}{3g}
levou 56 s
Como pensou
**Analyzing the Scenario**
I'm currently focused on dissecting the provided problem statement, specifically the oblique launch scenario. I've noted the assumption for small angles and how it might apply. My next step is to formulate the initial conditions and identify the key physical principles, like projectile motion and, potential simplification using the small angle assumption.
**Deconstructing the Problem**
I'm now zeroing in on the specific details of this oblique launch scenario, with the provided initial conditions and coefficient of restitution. I'm carefully breaking down the problem into its components. I have identified the constant horizontal velocity due to the smooth surface and am now focused on analyzing the vertical motion, considering the impact of the coefficient of restitution on each bounce.
**Calculating Bounce Heights**
I've determined the vertical velocity before the first impact as $-v_{y0}$, and after the first impact as $v_{y1} = e * v_{y0}$. Extending this, the initial vertical velocity for the (n+1)th bounce is $v_{yn} = e^n * v_{y0}$, and I'm using this to find the maximum height after the nth bounce: $H_n = v_{yn}^2 / (2g)$. With the coefficient of restitution and initial velocity, I have expressed this as $H_n = (V^2 / (8g)) * (0.7)^{2n}$ or $H_n = (V^2 / (8g)) * (0.49)^n$.
**Determining the Minimum Energy**
I've clarified that the minimum energy occurs when the vertical motion ceases, and thus $v_y$ is zero. The constant horizontal velocity means the minimum energy is solely the kinetic energy associated with the horizontal motion: $\frac{1}{2} m v_x^2$. This means, effectively, the ball is sliding horizontally without bouncing. It makes sense, as the bounces are the only dissipating element in the system.
**Calculating Total Time**
I've determined the total time for the infinite bounces. The initial flight time is $T_0 = V/g$, and the time between the *k*-th and *(k+1)*-th impact is $T_k = e^k T_0$. Therefore, the total time is a geometric series, summing to $T_{\text{total}} = T_0/(1-e)$, which leads to $T_{\text{total}} = (10V)/(3g)$ when substituting values. I am now rethinking the wording of "minimum energy" to confirm its timing. I am now exploring if the mechanical energy is conserved between impacts.
**Revising Energy Considerations**
I'm now refining my understanding of energy throughout the bouncing process, acknowledging its discontinuity at impact. After each impact, mechanical energy decreases, with the minimum value asymptotically approaching the kinetic energy from horizontal motion. Therefore, the minimum energy is indeed reached when vertical motion fully ceases, aligning with the infinitely many bounces and also the previous result, giving me confidence in it. I'm now also considering alternative interpretations of "energy" such as kinetic energy at the apex of motion.
**Clarifying Energy Definitions**
I'm now focusing on the subtle distinction between *kinetic energy* at the apex of each bounce versus the overall *mechanical energy* of the system. I'm taking a critical look at the problem statement's wording, "the minimum *of* its energy," which points me towards considering the total mechanical energy, which is dissipated with each inelastic collision. This is distinct from the minimum kinetic energy at each bounce's apex. The instruction at the top is not applicable for this part of the thought process.
**Interpreting Exam Instructions**
I've realized the "small angle" approximation is likely a general instruction from the exam's header, rather than specific to this problem. The given angle, $30^\circ$, doesn't warrant the approximation. I've re-examined potential applications, such as the angle of impact after bounces, but it doesn't apply to the questions in the provided scenario.
**Defining Initial Conditions**
I'm now precisely defining the initial conditions based on the problem statement, specifically the launch angle and initial velocity. I have determined the initial horizontal and vertical velocity components. The smooth horizontal surface simplifies things; the horizontal velocity remains constant, and any impulses during collisions will act solely in the vertical direction. I am focusing on making the velocities precise now.
**Calculating Bounce Heights**
I've determined the height after the nth bounce with precision, confirming $H_n = \frac{V^2}{8g} (0.49)^n$. This confirms my previous equations based on the coefficient of restitution and initial vertical velocity, which has also been double-checked for accuracy.
**Refining Energy Concepts**
My focus is now on the *minimum* energy, which I interpret as the total mechanical energy of the system, not just kinetic. It diminishes with each bounce due to inelastic collisions. I can confirm this is reached when vertical motion fully ceases and only horizontal kinetic energy remains, which supports the previous calculations. The phrasing "minimum of its energy" guides me towards considering total mechanical energy.
**Calculating the Total Time**
I've precisely calculated the time interval. My analysis confirms the total time from launch to minimum energy is $\Delta t = \frac{10V}{3g}$, derived from the infinite sum of flight times between bounces. This result, consistent with my earlier findings, provides a clear timeline for the energy dissipation process.
**Formulating the Response**
I'm now drafting a concise response suitable for the ITA exam format. I'm starting by decomposing the initial velocity into horizontal and vertical components, and also noting the smooth surface means horizontal velocity remains constant. The vertical component is key to analyzing each bounce. I am confirming previous calculations and ensuring a clear, organized structure.
**Confirming Velocity & Energy**
I've precisely calculated the vertical velocities before and after each bounce, incorporating the coefficient of restitution, leading to $v_{yn} = (0.7)^n V/2$. This allows me to confirm the maximum height after the nth bounce as $H_n = V^2 / (8g) * (0.49)^n$. Regarding minimum energy, the analysis confirms its minimum state at $E_{\text{min}} = 3/8 mV^2$, when vertical motion stops after infinite bounces.
Para a resolução do problema, adotamos um sistema de coordenadas cartesiano com a origem no ponto de lançamento, eixo x horizontal ao longo do solo e eixo y vertical apontando para cima.
A velocidade inicial da massa m é dada por:
v_{x0} = V \cos 30^\circ = \frac{\sqrt{3}}{2} V
v_{y0} = V \operatorname{sen} 30^\circ = \frac{V}{2}
Como a superfície horizontal é perfeitamente lisa, não há forças dissipativas na direção horizontal (a força impulsiva durante as colisões atua exclusivamente na direção vertical, perpendicular ao solo). Portanto, a componente horizontal da velocidade permanece constante durante todo o movimento:
v_x(t) = v_{x0} = \frac{\sqrt{3}}{2} V
a) Altura máxima após n choques
Na ausência de resistência do ar, o módulo da velocidade vertical com que a massa atinge o solo em uma dada colisão é igual ao módulo da velocidade com que ela iniciou o salto correspondente.
Pela definição do coeficiente de restituição e = 0,7 para colisões contra uma superfície fixa:
v_{y,\text{após}} = e \cdot v_{y,\text{antes}}
Dessa forma, a componente vertical da velocidade imediatamente após o n-ésimo choque (v_{yn}) é dada por:
v_{yn} = e^n v_{y0} = (0,7)^n \left(\frac{V}{2}\right)
A altura máxima H_n atingida na trajetória parabólica subsequente ao n-ésimo choque ocorre quando a componente vertical da velocidade se anula (v_y = 0):
v_y^2 = v_{yn}^2 - 2g H_n \implies 0 = v_{yn}^2 - 2g H_n
H_n = \frac{v_{yn}^2}{2g} = \frac{\left[(0,7)^n \frac{V}{2}\right]^2}{2g} = \frac{V^2}{8g} (0,7)^{2n} = \frac{V^2}{8g} (0,49)^n
b) Intervalo de tempo para que a massa m atinja o mínimo da sua energia
A energia mecânica da massa ao longo de sua trajetória é dada por:
E = E_c + E_p = \frac{1}{2}m v_x^2 + \left(\frac{1}{2}m v_y^2 + mgy\right)
Como v_x é constante e o solo está no nível de referência y = 0, a energia mecânica atinge o seu valor mínimo absoluto quando a componente do movimento vertical cessa por completo (y = 0 e v_y = 0). Nesse estado, resta apenas a energia cinética do movimento horizontal:
E_{\text{mín}} = \frac{1}{2}m v_x^2 = \frac{3}{8}mV^2
Essa condição é atingida após infinitas colisões sucessivas (n \to \infty).
O tempo de voo antes do primeiro choque é:
T_0 = \frac{2 v_{y0}}{g} = \frac{2(V/2)}{g} = \frac{V}{g}
O tempo de voo entre o k-ésimo e o (k+1)-ésimo choque é:
T_k = \frac{2 v_{yk}}{g} = \frac{2 e^k v_{y0}}{g} = e^k T_0
O intervalo de tempo total decorrido desde o lançamento até a extinção do movimento vertical é dado pela soma da série geométrica infinita:
\Delta t = \sum_{k=0}^{\infty} T_k = T_0 \sum_{k=0}^{\infty} e^k = T_0 \left(\frac{1}{1 - e}\right)
Substituindo os valores de T_0 = \frac{V}{g} e e = 0,7:
\Delta t = \frac{V}{g} \left(\frac{1}{1 - 0,7}\right) = \frac{V}{g} \left(\frac{1}{0,3}\right) = \frac{10 V}{3 g}
Resposta final: a) \frac{V^2}{8g}(0,49)^n; b) \frac{10V}{3g}
Respondeu · bate com a resposta de referência dos cursinhos
a) (0,49)^n V²/(8g); b) 10V/(3g)
levou 38 s
Como pensou
**Analyzing Physics Problem**
I am currently processing the initial details of an oblique projectile motion problem from a physics exam. My focus is on meticulously dissecting the problem statement, particularly the given initial velocity and angle of launch. This initial understanding is crucial for setting up the correct physics framework.
**Calculating Projectile Rebounds**
I'm now focused on calculating the maximum height after multiple collisions in this oblique projectile motion scenario. I've established the initial vertical velocity and derived a formula for the vertical velocity after the $n$-th impact using the coefficient of restitution. This is key to determining the subsequent maximum heights.
**Deriving Projectile Height**
I've successfully derived the formula for the maximum height after the n-th collision, $h_n$, as $(0.49)^n \frac{V^2}{8g}$, and I'll present both $(0.7)^{2n}$ and $(0.49)^n$ forms for clarity. I'm now beginning to analyze the time to reach minimum energy in item b).
**Investigating Energy Minimum**
I'm re-evaluating the concept of minimum energy. Initially, I considered kinetic energy, but I now believe the problem refers to mechanical energy. This minimum is achieved as the vertical velocity approaches zero, after an infinite number of bounces, with the total mechanical energy converging to the horizontal kinetic energy component.
**Calculating Total Time**
I am now calculating the total time for the projectile's vertical motion to cease after an infinite number of bounces, using the geometric series summation. I've confirmed that this total time is $\Delta t = \frac{10V}{3g}$ with $e=0.7$. I'm also considering the phrasing of "energia" to ensure consistency with common physics problem conventions.
**Analyzing Energy Minimization**
I am now definitively concluding that the problem refers to mechanical energy. My prior calculations for the time to reach this minimum, using a geometric series summation, were correct for an infinite number of bounces where the vertical velocity becomes zero, resulting in the minimum energy being solely the horizontal kinetic energy. The phrasing in Portuguese aligns with this interpretation.
**Summing Flight Times**
I'm now calculating the total flight duration by summing the individual bounce times. I've established that the time for each successive flight follows a geometric progression, which I'm summing to infinity. This will give me the total time until the projectile's vertical motion ceases.
a) A componente vertical da velocidade inicial de lançamento é dada por:
V_{y0} = V \operatorname{sen} 30^\circ = \frac{V}{2}
A cada colisão com o solo horizontal, o módulo da componente vertical da velocidade imediatamente após o impacto passa a ser multiplicado pelo coeficiente de restituição e = 0,7. Dessa forma, imediatamente após o n-ésimo choque, a velocidade vertical será:
V_{yn} = e^n V_{y0} = (0,7)^n \frac{V}{2}
Aplicando a equação de Torricelli no movimento vertical após o n-ésimo choque (0 = V_{yn}^2 - 2gh_n), obtemos a altura máxima h_n:
h_n = \frac{V_{yn}^2}{2g} = \frac{\left[(0,7)^n \frac{V}{2}\right]^2}{2g} \implies h_n = (0,7)^{2n} \frac{V^2}{8g} = (0,49)^n \frac{V^2}{8g}
b) Como a superfície horizontal é perfeitamente lisa, não há forças dissipativas na direção horizontal e a componente horizontal da velocidade (V_x = V \cos 30^\circ) permanece constante durante todo o movimento. A energia mecânica da massa m é dissipada exclusivamente durante os choques inelásticos com o solo. Assim, a energia mecânica atinge o seu valor mínimo quando o movimento vertical cessa completamente (n \to \infty, de modo que V_{yn} \to 0) e a partícula passa apenas a deslizar sobre o plano horizontal.
O tempo de voo desde o lançamento até o primeiro choque é:
\Delta t_0 = \frac{2V_{y0}}{g} = \frac{2(V/2)}{g} = \frac{V}{g}
Analogamente, o tempo de voo entre o k-ésimo e o (k+1)-ésimo choque é:
\Delta t_k = \frac{2V_{yk}}{g} = e^k \frac{2V_{y0}}{g} = e^k \Delta t_0
O intervalo de tempo total \Delta t necessário para que cessem as colisões é dado pela soma dos termos de uma progressão geométrica infinita de razão e = 0,7:
\Delta t = \sum_{k=0}^{\infty} \Delta t_k = \Delta t_0 (1 + e + e^2 + \dots) = \frac{\Delta t_0}{1 - e}
Substituindo os valores na expressão acima, temos:
\Delta t = \frac{V/g}{1 - 0,7} = \frac{V}{0,3g} \implies \Delta t = \frac{10V}{3g}
Resposta final: a) (0,49)^n V²/(8g); b) 10V/(3g)
Respondeu · bate com a resposta de referência dos cursinhos
a) \dfrac{V^2}{8g}(0{,}7)^{2n}; b) \dfrac{10V}{3g}.
levou 22 s
Como pensou
A componente horizontal da velocidade permanece constante, pois o solo é liso:
v_x=V\cos30^\circ=\frac{\sqrt3\,V}{2}.
A componente vertical inicial é v_{y0}=V\sen30^\circ=V/2.
a) A cada choque, o módulo da componente vertical da velocidade é multiplicado pelo coeficiente de restituição e=0{,}7. Assim, imediatamente após o n-ésimo choque,
v_{yn}=0{,}7^n\frac V2.
Usando v_y^2=v_{yn}^2-2gh, a altura máxima atingida após esse choque é
h_n=\frac{v_{yn}^2}{2g}
=\frac{V^2}{8g}(0{,}7)^{2n}.
b) Tomando a energia potencial nula no solo, a energia mecânica após o n-ésimo choque é
E_n=\frac{m}{2}\left(v_x^2+v_{yn}^2\right)
=\frac{mV^2}{8}\left[3+(0{,}7)^{2n}\right].
Ela tende ao mínimo 3mV^2/8 após infinitos choques. O tempo do lançamento até o primeiro choque é V/g; depois do n-ésimo choque, o tempo até o choque seguinte é (V/g)(0{,}7)^n. Portanto, o tempo total até o limite é
T=\frac Vg\sum_{n=0}^{\infty}(0{,}7)^n
=\frac Vg\frac{1}{1-0{,}7}
=\frac{10V}{3g}.
Resposta final: a) \dfrac{V^2}{8g}(0{,}7)^{2n}; b) \dfrac{10V}{3g}.