| 1 It's noticed that the same current flows through all elements | 0.20 |
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| 2 \[U_1 = \mathcal{E}\frac{\lambda h}{\lambda a + R_0}\] | 0.20 |
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| 3 \[V = a^3 \frac{U_1}{\mathcal{E}} \left( 1 + \frac{R_0}{\lambda a} \right)\] | 0.20 |
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| 1 The readings of the voltmeter $U_2$ is written using the difference of the potentials | 0.40 |
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| 2 \[ U_2 = \mathcal{E} \left( \frac{h}{a} - \frac{R_1}{R_1 + R_2} \right) \] | 0.40 |
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| 3 \[ V= a^3 \left( \frac{U_2}{\mathcal{E}} + \frac{R_1/R_2}{R_1/R_2 + 1} \right)\] | 0.20 |
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| 1 It's written that a deviated value of $R_1/R_2$ doesn't change the slope | 0.40 |
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| 2 It's determined that $V_0=76~\text{dm}^3$ | 0.40 |
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| 3 A method of determinig $R_1/R_2$ is proposed, e.g. readings when $t=0$ | 0.40 |
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| 4 \[R_1/R_2 = 23/15 \approx 1.53\] | 0.40 |
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| 1 The graph is a parabola with downward branches | 0.20 |
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| 2 The parabola goes from $(0,0)$ to $(\omega_0,0)$ | 0.20 |
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| 3 The graph is a horizontal line $\eta=0$ | 0.20 |
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| 1 It's written that $dW = M d \theta$ or analogous equation | 0.50 |
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1
The substitution is made \[ M\omega = \eta P_0\] |
0.50 |
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| 2 \[ M = \frac{\alpha P_0 }{\omega_0} \left( 1 - \frac{\omega}{\omega_0} \right)\] | 0.50 |
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| 1 \[\omega_W = \omega k\] | 0.30 |
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| 2 \[ \omega M = \omega_W M_W \] | 0.50 |
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| 3 \[ M_W = \frac{M}{k}\] | 0.40 |
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1
Relation between powers \[ \eta P_0 = \beta v^2 \]or the 2nd Newton's law \[ \frac{M_W}{r} = \beta v\]is written |
0.60 |
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| 2 The substitution $v = k \omega r$ is made | 0.20 |
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| 3 \[v = \omega_0 r \frac{1}{\frac{1}{k} + k \frac{\beta r^2 \omega_0^2}{\alpha P_0}}\] | 0.60 |
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| 4 The graph is linear for low values of $k$ | 0.50 |
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| 5 The graph is hyperbolic for high values of $k$ | 0.50 |
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| 1 To determine $k_\text{max}$ the derivative is proposed | 0.20 |
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2
The derivative is calculated: \[ \left( \frac{a}{k} + bk \right)' = -\frac{a}{k^2} + b\] |
0.40 |
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| 3 \[k_\text{max} = \sqrt{\frac{\alpha P_0}{\beta r^2 \omega_0^2}}\] | 0.50 |
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