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发表于 2025-9-20 09:55:23|字数:5,127
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三一班赵婧彤 发表于 2025-9-20 09:53
Of course. The image shows a classic physics problem involving a block on an inclined plane. Here is a detailed, step-by-step solution.
### Problem Summary:
A block of mass **m = 2.5 kg** is placed on a plane inclined at an angle **θ = 25°** to the horizontal. A force **F = 18 N** is applied to the block, parallel to the incline and directed **up the incline**. The coefficient of kinetic friction between the block and the plane is **μ_k = 0.15**. The block moves a distance **d = 2.0 m** up the incline. We are asked to find the **work done by the gravitational force** (W_grav) and the **work done by the friction force** (W_fric).
---
### Step 1: Visualize and Draw a Free-Body Diagram
The forces acting on the block are:
1. **Gravitational Force (mg):** Acts straight downward.
2. **Applied Force (F = 18 N):** Directed up the incline.
3. **Normal Force (N):** Perpendicular to the surface of the incline.
4. **Kinetic Friction Force (f_k):** Opposes the motion. Since the block is moving *up* the incline, the friction force acts *down* the incline.
[asy]
unitsize(0.8cm);
// Draw the inclined plane
draw((0,0)--(8,0), black+1.5);
draw((0,0)--(6,3), black+1.5);
label("$\theta$", (1.5,0), NE);
// Draw the block as a rectangle
path block = shift(4,2) * rotate(atan(3/6)) * box((0,0), (1,0.5));
fill(block, lightgray);
draw(block, black+1);
// Draw and label forces
// Gravity
draw((4,2)--(4,0.5), red, Arrow);
label("$mg$", (4, 1.25), W);
// Normal
pair center = (4,2);
pair normDir = dir(90-atan(3/6));
draw(center--(center+1.5*normDir), blue, Arrow);
label("$N$", center+1.5*normDir, normDir);
// Applied Force (F) - up the incline
pair upIncline = dir(atan(3/6));
draw(center--(center+2*upIncline), green, Arrow);
label("$F$", center+2*upIncline, upIncline);
// Friction Force (f_k) - down the incline
pair downIncline = dir(atan(3/6)+180);
draw(center--(center+1*downIncline), magenta, Arrow);
label("$f_k$", center+1*downIncline, downIncline);
// Angle arc for theta
draw(arc((0,0), 1, 0, atan(3/6)), black);
[/asy]
---
### Step 2: Resolve the Gravitational Force (mg)
The gravitational force has a component parallel to the incline and a component perpendicular to the incline.
* **Parallel Component (down the incline):** $mg\sin\theta$
* **Perpendicular Component (into the incline):** $mg\cos\theta$
These components are crucial for finding the normal force and the work done by gravity.
---
### Step 3: Calculate the Work Done by Gravity (W_grav)
**Formula for work:** $W = F \cdot d \cdot \cos\phi$
where $\phi$ is the angle between the force vector and the displacement vector.
* **Force:** Gravitational force, $mg$ (magnitude = $2.5 \times 9.8 = 24.5$ N)
* **Displacement:** $d = 2.0$ m, directed *up the incline*.
* **Angle between vectors:** The gravitational force acts vertically downward. The displacement is at an angle of $25°$ above the horizontal. Therefore, the angle $\phi$ between the force vector (down) and the displacement vector (25° up from horizontal) is:
$\phi = 90° + 25° = 115°$
*(You can also find this by noting that the angle between downward and upward along the incline is 180°, so the angle between downward and *up-the-incline* is 180° - 25° = 155°. However, the standard method using the incline angle is simpler).*
A more straightforward way is to use the component we found earlier. The work done by gravity will be equal to the work done by its component *parallel to the displacement*.
$W_{\text{grav}} = (-\text{mg}\sin\theta) \times d$
The negative sign is crucial because the component of gravity parallel to the incline ($mg\sin\theta$) acts *down* the incline, which is *opposite* to the displacement direction (*up* the incline).
Let's calculate:
1. $mg = 2.5 \, \text{kg} \times 9.8 \, \text{m/s}^2 = 24.5 \, \text{N}$
2. $\sin(25°) \approx 0.4226$
3. $mg\sin\theta = 24.5 \times 0.4226 \approx 10.354 \, \text{N}$ (down the incline)
4. Since force and displacement are in opposite directions:
$W_{\text{grav}} = - (mg\sin\theta) \times d = - (10.354 \, \text{N}) \times (2.0 \, \text{m})$
$W_{\text{grav}} \approx -20.71 \, \text{J}$
**The work done by gravity is approximately -20.7 Joules.**
---
### Step 4: Calculate the Work Done by Friction (W_fric)
**Formula for work:** $W = f_k \cdot d \cdot \cos\phi$
Again, $\phi$ is the angle between the friction force and the displacement.
* **Displacement:** $d = 2.0$ m, up the incline.
* **Friction Force (f_k):** We need to find its magnitude. The formula is $f_k = \mu_k N$.
* **Direction:** The friction force acts *down* the incline, opposite to the motion.
**First, find the Normal Force (N):**
Since there is no acceleration perpendicular to the incline, the net force in that direction is zero.
Forces in the perpendicular direction:
1. Normal Force (N): out of the incline (positive).
2. Perpendicular component of gravity ($mg\cos\theta$): into the incline (negative).
$\sum F_{\perp} = 0$
$N - mg\cos\theta = 0$
$N = mg\cos\theta$
Now calculate N:
1. $\cos(25°) \approx 0.9063$
2. $mg\cos\theta = 24.5 \times 0.9063 \approx 22.204 \, \text{N}$
3. So, $N = 22.204 \, \text{N}$
**Now find the Kinetic Friction Force (f_k):**
$f_k = \mu_k N = 0.15 \times 22.204 \, \text{N} \approx 3.331 \, \text{N}$
This force acts *down* the incline.
**Finally, calculate the work done by friction:**
The displacement is *up* the incline. The friction force is *down* the incline. The angle between them is $180°$. Since $\cos(180°) = -1$, the work will be negative.
$W_{\text{fric}} = f_k \times d \times \cos(180°) = (3.331 \, \text{N}) \times (2.0 \, \text{m}) \times (-1)$
$W_{\text{fric}} \approx -6.662 \, \text{J}$
**The work done by friction is approximately -6.7 Joules.**
---
### Final Answers
* **Work done by the gravitational force, $W_{\text{grav}}$:** $\boxed{-21 \text{ J}}$ (Rounded to two significant figures, as appropriate for the given data: $d = 2.0$ m has two significant figures).
* **Work done by the friction force, $W_{\text{fric}}$:** $\boxed{-6.7 \text{ J}}$
--来源:越嘉艺术网 |
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