Question: In the given figure, PQRS is a square in which PR = 10 cm. PS is produced to T. What is the area of \(\Delta QRT\) so formed? Find it.
1. **Problem Statement:**
Given a square \(PQRS\) with diagonal \(PR = 10\) cm, and \(PS\) extended to point \(T\), find the area of triangle \(\Delta QRT\).
2. **Understanding the figure and properties:**
- Since \(PQRS\) is a square, all sides are equal and all angles are \(90^\circ\).
- The diagonal \(PR\) of a square relates to the side length \(s\) by the formula:
$$PR = s\sqrt{2}$$
3. **Calculate the side length \(s\) of the square:**
$$s = \frac{PR}{\sqrt{2}} = \frac{10}{\sqrt{2}} = 5\sqrt{2}$$
4. **Coordinates assignment for clarity:**
Assume the square is placed on the coordinate plane for easier calculation:
- Let \(P = (0,0)\)
- Since \(PQRS\) is a square, let \(Q = (s,0) = (5\sqrt{2},0)\)
- \(R = (s,s) = (5\sqrt{2},5\sqrt{2})\)
- \(S = (0,s) = (0,5\sqrt{2})\)
5. **Point \(T\) lies on the line extending \(PS\):**
- \(PS\) is vertical from \(P(0,0)\) to \(S(0,5\sqrt{2})\).
- Extending \(PS\) beyond \(S\) means \(T\) has coordinates \((0,y)\) with \(y > 5\sqrt{2}\).
6. **Find coordinates of \(T\):**
- Since \(T\) lies on the extension of \(PS\), let \(T = (0,t)\) where \(t > 5\sqrt{2}\).
7. **Calculate area of \(\Delta QRT\):**
- Points are \(Q = (5\sqrt{2},0)\), \(R = (5\sqrt{2},5\sqrt{2})\), and \(T = (0,t)\).
- Area of triangle with vertices \((x_1,y_1), (x_2,y_2), (x_3,y_3)\) is:
$$\text{Area} = \frac{1}{2} \left| x_1(y_2 - y_3) + x_2(y_3 - y_1) + x_3(y_1 - y_2) \right|$$
Substitute:
$$= \frac{1}{2} | 5\sqrt{2}(5\sqrt{2} - t) + 5\sqrt{2}(t - 0) + 0(0 - 5\sqrt{2}) |$$
Simplify inside:
$$= \frac{1}{2} | 5\sqrt{2} \times 5\sqrt{2} - 5\sqrt{2} t + 5\sqrt{2} t | = \frac{1}{2} | 5\sqrt{2} \times 5\sqrt{2} |$$
Since \(-5\sqrt{2} t + 5\sqrt{2} t = 0\),
Calculate \(5\sqrt{2} \times 5\sqrt{2} = 25 \times 2 = 50\),
So area = \(\frac{1}{2} \times 50 = 25\).
8. **Final answer:**
The area of \(\Delta QRT\) is \(25\) square centimeters.
**Note:** The area is independent of the exact position of \(T\) on the extension of \(PS\) because the terms involving \(t\) cancel out.