In a damped harmonic oscillator, the amplitude decreases over time due to the energy lost to damping forces.

In a damped harmonic oscillator, the amplitude decreases over time due to the loss of energy.

The damping coefficient determines the rate of energy loss in a damped harmonic oscillator.

The damping coefficient determines how quickly energy is lost in a damped harmonic oscillator.

Using E(t) = E_0 e^(-2ζω_nt), we find ζ = 0.2.

In a Daniell cell, Zinc acts as the anode.

In a Daniell cell, zinc is oxidized.

Since the mean is greater than the median, the data is skewed right.

Since the mean is greater than the median, the data is skewed to the right.

Since the mean is greater than the median, the data is skewed right.

Number of values = Sum / Mean = 500 / 50 = 10.

Since the mean is greater than the mode, the data is positively skewed.

Mode = 4 (most frequently occurring value).

Coefficient of Variation = (Standard Deviation / Mean) * 100 = (2/10) * 100 = 20%.

Since the mean is greater than the median, the data is skewed right.

Since the mean is greater than the median, the data is positively skewed.

Coefficient of Variation = (Standard Deviation / Mean) * 100 = (4/20) * 100 = 20%.

Sum = Mean * Number of Observations = 50 * 10 = 500.

Q1 = 2, Q3 = 4. Interquartile Range = Q3 - Q1 = 4 - 2 = 2.

There are 26 red cards (hearts and diamonds). The number of hearts is 13. Thus, P(Heart | Red) = 13/26 = 1/2.

There are 26 red cards (hearts and diamonds). The number of hearts is 13. Thus, P(Heart | Red) = 13/26 = 1/2.

Increasing the number of slits increases the sharpness of the maxima, thus decreasing the angular width.

Increasing the number of slits increases the intensity of the maxima due to constructive interference.

Increasing the number of slits in a diffraction grating increases the sharpness of the maxima due to constructive interference.

The angle of diffraction is directly proportional to the order of the maximum in a diffraction grating.

In a diffraction pattern, the minima are always darker than the maxima, which have higher intensity.

Using the condition for the first minimum a sin(30°) = λ, we find the ratio a/λ = 1/√3.

The intensity of the central maximum is theoretically infinite compared to the first minimum, which has zero intensity.

The intensity of the central maximum in a diffraction pattern is at its maximum compared to other maxima.

The intensity of the central maximum in a diffraction pattern depends on both the wavelength of light and the slit width.