Because of overloading, the power of a heater connected
Because of overloading, the power of a heater connected to a network of voltage $U_{1} = 220\ \text{V}$ drops from $P_{1} = 1000\ \text{W}$ to $P_{2} = 800\ \text{W}$. Find the drop in the network voltage, assuming the resistance $R$ stays constant.
Explanation of Method
Inverting the differential relation to estimate a cause from its effect.
Step 1: The relation between power and voltage
With constant resistance, $P = \frac{U^{2}}{R}$.
Step 2: Find $R$ from the initial state
\[ R = \frac{U_{1}^{2}}{P_{1}} = \frac{220^{2}}{1000} = \frac{48400}{1000} = 48.4\ \Omega. \]
Step 3: Differentiate and invert
\[ \frac{dP}{dU} = \frac{2U}{R} \;\Longrightarrow\; \Delta P \approx \frac{2U_{1}}{R}\,\Delta U \;\Longrightarrow\; \Delta U \approx \frac{R\,\Delta P}{2U_{1}}. \]
This is the differential used backwards: the observed change in the effect $P$ is converted into an estimate of the change in the cause $U$.
Step 4: Substitute the numbers
\[ \Delta P = P_{2}-P_{1} = 800-1000 = -200\ \text{W}, \]
\[ \Delta U \approx \frac{48.4\cdot(-200)}{2\cdot 220} = \frac{-9680}{440} = -22\ \text{V}. \]
The minus sign says the voltage fell.
Step 5: Verification — and the size of the error
Here the exact answer is available, since $U = \sqrt{RP}$: \[U_{2} = \sqrt{48.4\cdot 800} = \sqrt{38720} = 220\sqrt{0.8} \approx 196.7740\ \text{V}\]
\[\Delta U_{\text{exact}} = 196.7740-220 = -23.2260\ \text{V}\]
\[\text{Error of the linear estimate: } 1.226\ \text{V}, \text{ i.e. about } 5.3\% \text{ of the true drop}\]
Result
Final answer:
\[\boxed{\,\bigl|\Delta U\bigr| \approx 22\ \text{V} \qquad\text{(from } 220\ \text{V to about } 198\ \text{V)}\,}\]
Remark
Remark. A $20\%$ fall in power is not a small increment, so the differential estimate is only fair here — it understates the drop by $1.2\ \text{V}$. Because $P$ is convex in $U$, the tangent line always lies below the curve for a decrease, so the linear estimate is guaranteed to understate. If the exact relation is used from the start, $U_{2} = U_{1}\sqrt{P_{2}/P_{1}} = 220\sqrt{0.8}$, no approximation is needed at all.